Optical image capturing system

ABSTRACT

The invention discloses a five-piece optical lens for capturing image and a five-piece optical module for capturing image. In order from an object side to an image side, the optical lens along the optical axis comprises a first lens with refractive power; a second lens with refractive power, a third lens with refractive power; a fourth lens with refractive power; a fifth lens with refractive power, and at least one of the image-side surface and object-side surface of each of the five lens elements is aspheric. The optical lens can increase aperture value and improve the imagining quality for use in compact cameras.

BACKGROUND OF THE INVENTION 1. Technical Field

The present invention relates generally to an optical system, and moreparticularly to a compact optical image capturing system for anelectronic device.

2. Description of Related Art

In recent years, with the rise of portable electronic devices havingcamera functionalities, the demand for an optical image capturing systemis raised gradually. The image sensing device of the ordinaryphotographing camera is commonly selected from charge coupled device(CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor).In addition, as advanced semiconductor manufacturing technology enablesthe minimization of the pixel size of the image sensing device, thedevelopment of the optical image capturing system towards the field ofhigh pixels. Therefore, the requirement for high imaging quality israpidly raised.

The conventional optical system of the portable electronic deviceusually has three or four lenses. However, the optical system is askedto take pictures in a dark environment, in other words, the opticalsystem is asked to have a large aperture. The conventional opticalsystem could not provide a high optical performance as required.

It is an important issue to increase the amount of light entering thelens. In addition, the modem lens is also asked to have severalcharacters, including high image quality.

BRIEF SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an opticalimage capturing system and an optical image capturing lens which usecombination of refractive powers, convex and concave surfaces offive-piece optical lenses (the convex or concave surface in thedisclosure denotes the geometrical shape of an image-side surface or anobject-side surface of each lens on an optical axis) to increase theamount of incoming light of the optical image capturing system, and toimprove imaging quality for image formation, so as to be applied tominimized electronic products.

In addition, when it comes to certain application of optical imaging,there will be a need to capture image via light sources with wavelengthsin both visible and infrared ranges, an example of this kind ofapplication is IP video surveillance camera, which is equipped with theDay & Night function. The visible spectrum for human vision haswavelengths ranging from 400 to 700 nm, but the image formed on thecamera sensor includes infrared light, which is invisible to human eyes.Therefore, under certain circumstances, an IR cut filter removable (ICR)is placed before the sensor of the IP video surveillance camera, inorder to ensure that only the light that is visible to human eyes ispicked up by the sensor eventually, so as to enhance the “fidelity” ofthe image. The ICR of the IP video surveillance camera can completelyfilter out the infrared light under daytime mode to avoid color cast;whereas under night mode, it allows infrared light to pass through thelens to enhance the image brightness. Nevertheless, the elements of theICR occupy a significant amount of space and are expensive, which impedeto the design and manufacture of miniaturized surveillance cameras inthe future.

The aspect of embodiment of the present disclosure directs to an opticalimage capturing system and an optical image capturing lens which utilizethe combination of refractive powers, convex surfaces and concavesurfaces of four lenses, as well as the selection of materials thereof,to reduce the difference between the imaging focal length of visiblelight and imaging focal length of infrared light, in order to achievethe near “confocal” effect without the use of ICR elements.

The term and its definition to the lens parameter in the embodiment ofthe present are shown as below for further reference.

The lens parameters related to the magnification of the optical imagecapturing system

The optical image capturing system can be designed and applied tobiometrics, for example, facial recognition. When the embodiment of thepresent disclosure is configured to capture image for facialrecognition, the infrared light can be adopted as the operationwavelength. For a face of about 15 centimeters (cm) wide at a distanceof 25-30 cm, at least 30 horizontal pixels can be formed in thehorizontal direction of an image sensor (pixel size of 1.4 micrometers(μm)). The linear magnification of the infrared light on the image planeis LM, and it meets the following conditions: LM≥0.0003, where LM=(30horizontal pixels)*(1.4 μm pixel size)/(15 cm, width of the photographedobject). Alternatively, the visible light can also be adopted as theoperation wavelength for image recognition. When the visible light isadopted, for a face of about 15 cm wide at a distance of 25-30 cm, atleast 50 horizontal pixels can be formed in the horizontal direction ofan image sensor (pixel size of 1.4 micrometers (μm)).

The lens parameter related to a length or a height in the lens:

For visible spectrum, the present invention may adopt the wavelength of555 nm as the primary reference wavelength and the basis for themeasurement of focus shift; for infrared spectrum (700-1300 nm), thepresent invention may adopt the wavelength of 850 nm as the primaryreference wavelength and the basis for the measurement of focus shift.

The optical image capturing system includes a first image plane and asecond image plane. The first image plane is an image plane specificallyfor the visible light, and the first image plane is located at aposition of the optical axis and the through-focus modulation transferrate (value of MTF) at the first spatial frequency has a maximum value;the second image plane is an image plane specifically for the infraredlight, and the second image plane is located at a position the opticalaxis and the through-focus modulation transfer rate (value of MTF) atthe first spatial frequency has a maximum value. The optical imagecapturing system also includes a first average image plane and a secondaverage image plane. The first average image plane is an image planespecifically for the visible light, and the first average image plane isperpendicular to the optical axis. The first average image plane isinstalled at the average position of the defocusing positions, where thevalues of MTF of the visible light at the central field of view, 0.3field of view, and the 0.7 field of view are at their respective maximumat the first spatial frequency. The second average image plane is animage plane specifically for the infrared light, and the second averageimage plane is perpendicular to the optical axis. The second averageimage plane is installed at the average position of the defocusingpositions, where the values of MTF of the infrared light at the centralfield of view, 0.3 field of view, and the 0.7 field of view are at theirrespective maximum at the first spatial frequency.

The aforementioned first spatial frequency is set to be half of thespatial frequency (half frequency) of the image sensor (sensor) used inthe present invention. For example, for an image sensor having the pixelsize of 1.12 μm or less, the quarter spatial frequency, half spatialfrequency (half frequency) and full spatial frequency (full frequency)in the characteristic diagram of modulation transfer function are atleast 110 cycles/mm, 220 cycles/mm and 440 cycles/mm, respectively.Lights of any field of view can be further divided into sagittal ray andtangential ray.

The focus shifts where the through-focus MTF values of the visiblesagittal ray at the central field of view, 0.3 field of view, and 0.7field of view of the optical image capturing system are at theirrespective maxima, are denoted by VSFS0, VSFS3, and VSFS7 (unit ofmeasurement: mm), respectively. The maximum values of the through-focusMTF of the visible sagittal ray at the central field of view, 0.3 fieldof view, and 0.7 field of view are denoted by VSMTF0, VSMTF3, andVSMTF7, respectively. The focus shifts where the through-focus MTFvalues of the visible tangential ray at the central field of view, 0.3field of view, and 0.7 field of view of the optical image capturingsystem are at their respective maxima, are denoted by VTFS0, VTFS3, andVTFS7 (unit of measurement: mm), respectively. The maximum values of thethrough-focus MTF of the visible tangential ray at the central field ofview, 0.3 field of view, and 0.7 field of view are denoted by VTMTF0,VTMTF3, and VTMTF7, respectively. The average focus shift (position) ofboth the aforementioned focus shifts of the visible sagittal ray atthree fields of view and focus shifts of the visible tangential ray atthree fields of view is denoted by AVFS (unit of measurement: mm), whichequals to the absolute value |(VSFS0+VSFS3+VSFS7+VTFS0+VTFS3+VTFS7)/6|.

The focus shifts where the through-focus MTF values of the infraredsagittal ray at the central field of view, 0.3 field of view, and 0.7field of view of the optical image capturing system are at theirrespective maxima, are denoted by ISFS0, ISFS3, and ISFS7 (unit ofmeasurement: mm), respectively. The average focus shift (position) ofthe aforementioned focus shifts of the infrared sagittal ray at threefields of view is denoted by AISFS (unit of measurement: mm). Themaximum values of the through-focus MTF of the infrared sagittal ray atthe central field of view, 0.3 field of view, and 0.7 field of view aredenoted by ISMTF0, ISMTF3, and ISMTF7, respectively. The focus shiftswhere the through-focus MTF values of the infrared tangential ray at thecentral field of view, 0.3 field of view, and 0.7 field of view of theoptical image capturing system are at their respective maxima, aredenoted by ITFS0, ITFS3, and ITFS7 (unit of measurement: mm),respectively. The average focus shift (position) of the aforementionedfocus shifts of the infrared tangential ray at three fields of view isdenoted by AITFS (unit of measurement: mm). The maximum values of thethrough-focus MTF of the infrared tangential ray at the central field ofview, 0.3 field of view, and 0.7 field of view are denoted by ITMTF0,ITMTF3, and ITMTF7, respectively. The average focus shift (position) ofboth of the aforementioned focus shifts of the infrared sagittal ray atthe three fields of view and focus shifts of the infrared tangential rayat the three fields of view is denoted by AIFS (unit of measurement:mm), which equals to the absolute value of|(ISFS0+ISFS3+ISFS7+ITFS0+ITFS3+ITFS7)/6|.

The focus shift (difference) between the focal points of the visiblelight and the infrared light at their central fields of view (RGB/IR) ofthe entire optical image capturing system (i.e. wavelength of 850 nmversus wavelength of 555 nm, unit of measurement: mm) is denoted by FS,which satisfies the absolute value |(VSFS0+VTFS0)/2−(ISFS0+ITFS0)/2|.The difference (focus shift) between the average focus shift of thevisible light in the three fields of view and the average focus shift ofthe infrared light in the three fields of view (RGB/IR) of the entireoptical image capturing system is denoted by AFS (i.e. wavelength of 850nm versus wavelength of 555 nm, unit of measurement: mm), which equalsto the absolute value of |AIFS−AVFS|.

A height for image formation of the optical image capturing system isdenoted by HOI. A height of the optical image capturing system isdenoted by HOS. A distance from the object-side surface of the firstlens to the image-side surface of the fifth lens is denoted by InTL. Adistance from the first lens to the second lens is denoted by IN12(instance). A central thickness of the first lens of the optical imagecapturing system on the optical axis is denoted by TP1 (instance).

The lens parameter related to a material in the lens:

An Abbe number of the first lens in the optical image capturing systemis denoted by NA1 (instance). A refractive index of the first lens isdenoted by Nd1 (instance).

The lens parameter related to a view angle in the lens:

A view angle is denoted by AF. Half of the view angle is denoted by HAF.A major light angle is denoted by MRA.

The lens parameter related to exit/entrance pupil in the lens:

An entrance pupil diameter of the optical image capturing system isdenoted by HEP. An exit pupil of the optical image capturing systemrefers to the image of the aperture stop imaged in the imaging spaceafter passing through the lens behind the aperture stop, and the exitpupil diameter is denoted by HXP. For any surface of any lens, a maximumeffective half diameter (EHD) is a perpendicular distance between anoptical axis and a crossing point on the surface where the incidentlight with a maximum viewing angle of the system passing the very edgeof the entrance pupil. For example, the maximum effective half diameterof the object-side surface of the first lens is denoted by EHD11, themaximum effective half diameter of the image-side surface of the firstlens is denoted by EHD12, the maximum effective half diameter of theobject-side surface of the second lens is denoted by EHD21, the maximumeffective half diameter of the image-side surface of the second lens isdenoted by EHD22, and so on.

The lens parameter related to an arc length of the shape of a surfaceand a surface profile:

For any surface of any lens, a profile curve length of the maximumeffective half diameter is, by definition, measured from a start pointwhere the optical axis of the belonging optical image capturing systempasses through the surface of the lens, along a surface profile of thelens, and finally to an end point of the maximum effective half diameterthereof. In other words, the curve length between the aforementionedstart and end points is the profile curve length of the maximumeffective half diameter, which is denoted by ARS. For example, theprofile curve length of the maximum effective half diameter of theobject-side surface of the first lens is denoted by ARS11, the profilecurve length of the maximum effective half diameter of the image-sidesurface of the first lens is denoted by ARS12, the profile curve lengthof the maximum effective half diameter of the object-side surface of thesecond lens is denoted by ARS21, the profile curve length of the maximumeffective half diameter of the image-side surface of the second lens isdenoted by ARS22, and so on.

For any surface of any lens, a profile curve length of a half of theentrance pupil diameter (HEP) is, by definition, measured from a startpoint where the optical axis of the belonging optical image capturingsystem passes through the surface of the lens, along a surface profileof the lens, and finally to a coordinate point of a perpendiculardistance where is a half of the entrance pupil diameter away from theoptical axis. In other words, the curve length between theaforementioned stat point and the coordinate point is the profile curvelength of a half of the entrance pupil diameter (HEP), and is denoted byARE. For example, the profile curve length of a half of the entrancepupil diameter (HEP) of the object-side surface of the first lens isdenoted by ARE11, the profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the first lens isdenoted by ARE12, the profile curve length of a half of the entrancepupil diameter (HEP) of the object-side surface of the second lens isdenoted by ARE21, the profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the second lens isdenoted by ARE22, and so on.

The lens parameter related to a depth of the lens shape:

A displacement from a point on the object-side surface of the fifthlens, which is passed through by the optical axis, to a point on theoptical axis, where a projection of the maximum effective semi diameterof the object-side surface of the fifth lens ends, is denoted by InRS51(the depth of the maximum effective semi diameter). A displacement froma point on the image-side surface of the fifth lens, which is passedthrough by the optical axis, to a point on the optical axis, where aprojection of the maximum effective semi diameter of the image-sidesurface of the fifth lens ends, is denoted by InRS52 (the depth of themaximum effective semi diameter). The depth of the maximum effectivesemi diameter (sinkage) on the object-side surface or the image-sidesurface of any other lens is denoted in the same manner.

The lens parameter related to the lens shape:

A critical point C is a tangent point on a surface of a specific lens,and the tangent point is tangent to a plane perpendicular to the opticalaxis and the tangent point cannot be a crossover point on the opticalaxis. By the definition, a distance perpendicular to the optical axisbetween a critical point C41 on the object-side surface of the fourthlens and the optical axis is HVT41 (instance), and a distanceperpendicular to the optical axis between a critical point C42 on theimage-side surface of the fourth lens and the optical axis is HVT42(instance). A distance perpendicular to the optical axis between acritical point C51 on the object-side surface of the fifth lens and theoptical axis is HVT51 (instance), and a distance perpendicular to theoptical axis between a critical point C52 on the image-side surface ofthe fifth lens and the optical axis is HVT52 (instance). A distanceperpendicular to the optical axis between a critical point on theobject-side or image-side surface of other lenses the optical axis isdenoted in the same manner.

The object-side surface of the fifth lens has one inflection point IF511which is nearest to the optical axis, and the sinkage value of theinflection point IF511 is denoted by SGI511 (instance). A distanceperpendicular to the optical axis between the inflection point IF511 andthe optical axis is HIF511 (instance). The image-side surface of thefifth lens has one inflection point IF521 which is nearest to theoptical axis, and the sinkage value of the inflection point IF521 isdenoted by SGI521 (instance). A distance perpendicular to the opticalaxis between the inflection point IF521 and the optical axis is HIF521(instance).

The object-side surface of the fifth lens has one inflection point IF512which is the second nearest to the optical axis, and the sinkage valueof the inflection point IF512 is denoted by SGI512 (instance). Adistance perpendicular to the optical axis between the inflection pointIF512 and the optical axis is HIF512 (instance). The image-side surfaceof the fifth lens has one inflection point IF522 which is the secondnearest to the optical axis, and the sinkage value of the inflectionpoint IF522 is denoted by SGI522 (instance). A distance perpendicular tothe optical axis between the inflection point IF522 and the optical axisis HIF522 (instance).

The object-side surface of the fifth lens has one inflection point IF513which is the third nearest to the optical axis, and the sinkage value ofthe inflection point IF513 is denoted by SGI513 (instance). A distanceperpendicular to the optical axis between the inflection point IF513 andthe optical axis is HIF513 (instance). The image-side surface of thefifth lens has one inflection point IF523 which is the third nearest tothe optical axis, and the sinkage value of the inflection point IF523 isdenoted by SGI523 (instance). A distance perpendicular to the opticalaxis between the inflection point IF523 and the optical axis is HIF523(instance).

The object-side surface of the fifth lens has one inflection point IF514which is the fourth nearest to the optical axis, and the sinkage valueof the inflection point IF514 is denoted by SGI514 (instance). Adistance perpendicular to the optical axis between the inflection pointIF514 and the optical axis is HIF514 (instance). The image-side surfaceof the fifth lens has one inflection point IF524 which is the fourthnearest to the optical axis, and the sinkage value of the inflectionpoint IF524 is denoted by SGI524 (instance). A distance perpendicular tothe optical axis between the inflection point IF524 and the optical axisis HIF524 (instance).

An inflection point, a distance perpendicular to the optical axisbetween the inflection point and the optical axis, and a sinkage valuethereof on the object-side surface or image-side surface of other lensesis denoted in the same manner.

The lens parameter related to an aberration:

Optical distortion for image formation in the optical image capturingsystem is denoted by ODT. TV distortion for image formation in theoptical image capturing system is denoted by TDT. Further, the range ofthe aberration offset for the view of image formation may be limited to50%-100% field. An offset of the spherical aberration is denoted by DFS.An offset of the coma aberration is denoted by DFC.

Transverse aberration on an edge of an aperture is denoted by STA, whichstands for STOP transverse aberration, and is used to evaluate theperformance of one specific optical image capturing system. Thetransverse aberration of light in any field of view can be calculatedwith a tangential fan or a sagittal fan. More specifically, thetransverse aberration caused when the longest operation wavelength(e.g., 650 nm or 656 nm) and the shortest operation wavelength (e.g.,470 nm or 486 nm) pass through the edge of the aperture can be used asthe reference for evaluating performance. The coordinate directions ofthe aforementioned tangential fan can be further divided into a positivedirection (upper light) and a negative direction (lower light). Thelongest operation wavelength which passes through the edge of theaperture has an imaging position on the image plane in a particularfield of view, and the reference wavelength of the mail light (e.g., 555nm or 587.5 nm) has another imaging position on the image plane in thesame field of view. The transverse aberration caused when the longestoperation wavelength passes through the edge of the aperture is definedas a distance between these two imaging positions. Similarly, theshortest operation wavelength which passes through the edge of theaperture has an imaging position on the image plane in a particularfield of view, and the transverse aberration caused when the shortestoperation wavelength passes through the edge of the aperture is definedas a distance between the imaging position of the shortest operationwavelength and the imaging position of the reference wavelength. Theperformance of the optical image capturing system can be consideredexcellent if the transverse aberrations of the shortest and the longestoperation wavelength which pass through the edge of the aperture andimage on the image plane in 0.7 field of view (i.e., 0.7 times theheight for image formation HOI) are both less than 20 μm or 20 pixels.Furthermore, for a stricter evaluation, the performance cannot beconsidered excellent unless the transverse aberrations of the shortestand the longest operation wavelength which pass through the edge of theaperture and image on the image plane in 0.7 field of view are both lessthan 10 μm or 10 pixels.

The optical image capturing system has a maximum image height HOI on theimage plane vertical to the optical axis. A transverse aberration at 0.7HOI in the positive direction of the tangential fan after the longestoperation wavelength passing through the edge of the aperture is denotedby PLTA; a transverse aberration at 0.7 HOI in the positive direction ofthe tangential fan after the shortest operation wavelength passingthrough the edge of the aperture is denoted by PSTA; a transverseaberration at 0.7 HOI in the negative direction of the tangential fanafter the longest operation wavelength passing through the edge of theaperture is denoted by NLTA; a transverse aberration at 0.7 HOI in thenegative direction of the tangential fan after the shortest operationwavelength passing through the edge of the aperture is denoted by NSTA;a transverse aberration at 0.7 HOI of the sagittal fan after the longestoperation wavelength passing through the edge of the aperture is denotedby SLTA; a transverse aberration at 0.7 HOI of the sagittal fan afterthe shortest operation wavelength passing through the edge of theaperture is denoted by SSTA.

The present invention provides an optical image capturing system, inwhich the fifth lens is provided with an inflection point at theobject-side surface or at the image-side surface to adjust the incidentangle of each view field and modify the ODT and the TDT. In addition,the surfaces of the fifth lens are capable of modifying the optical pathto improve the imagining quality.

The optical image capturing system of the present invention includes afirst lens, a second lens, a third lens, a fourth lens, a fifth lens, afirst image plane, and a second image plane. The first image plane is animage plane specifically for the visible light, and the first imageplane is located at a position of the optical axis and the through-focusmodulation transfer rate (value of MTF) at the first spatial frequencyhas a maximum value; the second image plane is an image planespecifically for the infrared light, and the second image plane islocated at a position the optical axis and the through-focus modulationtransfer rate (value of MTF) at the first spatial frequency has amaximum value. All lenses among the first lens to the fifth lens haverefractive power. The first lens has refractive power. Both theobject-side surface and the image-side surface of the fifth lens areaspheric surfaces. The optical image capturing system satisfies:1≤f/HEP≤10; 0 deg<HAF≤150 deg; and |FS|≤60 μm; where f1, f2, f3, f4, andf5 are the focal lengths of the first, the second, the third, thefourth, the fifth lenses, respectively; f is a focal length of theoptical image capturing system; HEP is an entrance pupil diameter of theoptical image capturing system; HOS is a distance between theobject-side surface of the first lens and the first image plane on theoptical axis; HAF is a half of a maximum view angle of the optical imagecapturing system; HOI is the maximum image height on the first imageplane perpendicular to the optical axis of the optical image capturingsystem; FS is the distance on the optical axis between the first imageplane and the second image plane.

The present invention further provides an optical image capturingsystem, including a first lens, a second lens, a third lens, a fourthlens, a fifth lens, a first image plane, and a second image plane. Thefirst image plane is an image plane specifically for the visible light,and the first image plane is located at a position of the optical axisand the through-focus modulation transfer rate (value of MTF) at thefirst spatial frequency has a maximum value; the second image plane isan image plane specifically for the infrared light, and the second imageplane is located at a position the optical axis and the through-focusmodulation transfer rate (value of MTF) at the first spatial frequencyhas a maximum value. The first lens has refractive power, and theobject-side surface thereof can be convex near the optical axis. Thesecond lens has refractive power. The third lens has refractive power.The fourth lens has refractive power. The fifth lens has refractivepower. At least one lens among the first lens to the fifth lens is madeof plastic. At least one lens among the first lens to the fifth lens haspositive refractive power. The optical image capturing system satisfies:1≤f/HEP≤10; 0 deg<HAF≤150 deg; 0.9≤2(ARE/HEP)≤2.0; and |FS|≤60 μm; wheref1, f2, f3, f4, and f5 are the focal lengths of the first, the second,the third, the fourth, the fifth lenses, respectively; f is a focallength of the optical image capturing system; HEP is an entrance pupildiameter of the optical image capturing system; HOS is a distancebetween the object-side surface of the first lens and the first imageplane on the optical axis; HAF is a half of a maximum view angle of theoptical image capturing system; HOI is the maximum image height on thefirst image plane perpendicular to the optical axis of the optical imagecapturing system; FS is the distance on the optical axis between thefirst image plane and the second image plane; ARE is a profile curvelength measured from a start point where the optical axis of thebelonging optical image capturing system passes through the surface ofthe lens, along a surface profile of the lens, and finally to acoordinate point of a perpendicular distance where is a half of theentrance pupil diameter away from the optical axis.

The present invention further provides an optical image capturingsystem, including a first lens, a second lens, a third lens, a fourthlens, a fifth lens, a first average image plane, and a second averageimage plane. The first average image plane is an image planespecifically for the visible light, and the first average image plane isperpendicular to the optical axis. The first average image plane isinstalled at the average position of the defocusing positions, where thevalues of MTF of the visible light at the central field of view, 0.3field of view, and the 0.7 field of view are at their respective maximumat the first spatial frequency. The second average image plane is animage plane specifically for the infrared light, and the second averageimage plane is perpendicular to the optical axis. The second averageimage plane is installed at the average position of the defocusingpositions, where the values of MTF of the infrared light at the centralfield of view, 0.3 field of view, and the 0.7 field of view are at theirrespective maximum at the first spatial frequency. The number of thelenses having refractive power in the optical image capturing system isfive. The first lens has refractive power. The second lens hasrefractive power. The third lens has refractive power. The fourth lenshas refractive power. The fifth lens has refractive power. At least onelens among the first lens to the fifth lens is made of plastic. Theoptical image capturing system satisfies: 1≤f/HEP≤10; 0 deg<HAF≤150 deg;0.9≤2(ARE/HEP)≤2.0; and |AFS|≤60 μm; where f1, f2, f3, f4, and f5 arethe focal lengths of the first, the second, the third, the fourth, thefifth lenses, respectively; f is a focal length of the optical imagecapturing system; HEP is an entrance pupil diameter of the optical imagecapturing system; HOS is a distance between the object-side surface ofthe first lens and the first average image plane on the optical axis;HAF is a half of a maximum view angle of the optical image capturingsystem; HOI is the maximum image height on the first average image planeperpendicular to the optical axis of the optical image capturing system;ARE is a profile curve length measured from a start point where theoptical axis of the belonging optical image capturing system passesthrough the surface of the lens, along a surface profile of the lens,and finally to a coordinate point of a perpendicular distance where is ahalf of the entrance pupil diameter away from the optical axis; AFS isthe distance between the first average image plane and the secondaverage image plane; FS is the distance on the optical axis between thefirst average image plane and the second average image plane.

For any surface of any lens, the profile curve length within theeffective half diameter affects the ability of the surface to correctaberration and differences between optical paths of light in differentfields of view. With longer profile curve length, the ability to correctaberration is better. However, the difficulty of manufacturing increasesas well. Therefore, the profile curve length within the effective halfdiameter of any surface of any lens has to be controlled. The ratiobetween the profile curve length (ARS) within the effective halfdiameter of one surface and the thickness (TP) of the lens, which thesurface belonged to, on the optical axis (i.e., ARS/TP) has to beparticularly controlled. For example, the profile curve length of themaximum effective half diameter of the object-side surface of the firstlens is denoted by ARS11, the thickness of the first lens on the opticalaxis is TP1, and the ratio between these two parameters is ARS11/TP1;the profile curve length of the maximum effective half diameter of theimage-side surface of the first lens is denoted by ARS12, and the ratiobetween ARS12 and TP1 is ARS12/TP1. The profile curve length of themaximum effective half diameter of the object-side surface of the secondlens is denoted by ARS21, the thickness of the second lens on theoptical axis is TP2, and the ratio between these two parameters isARS21/TP2; the profile curve length of the maximum effective halfdiameter of the image-side surface of the second lens is denoted byARS22, and the ratio between ARS22 and TP2 is ARS22/TP2. For any surfaceof other lenses in the optical image capturing system, the ratio betweenthe profile curve length of the maximum effective half diameter thereofand the thickness of the lens which the surface belonged to is denotedin the same manner.

For any surface of any lens, the profile curve length within a half ofthe entrance pupil diameter (HEP) affects the ability of the surface tocorrect aberration and differences between optical paths of light indifferent fields of view. With longer profile curve length, the abilityto correct aberration is better. However, the difficulty ofmanufacturing increases as well. Therefore, the profile curve lengthwithin a half of the entrance pupil diameter (HEP) of any surface of anylens has to be controlled. The ratio between the profile curve length(ARE) within a half of the entrance pupil diameter (HEP) of one surfaceand the thickness (TP) of the lens, which the surface belonged to, onthe optical axis (i.e., ARE/TP) has to be particularly controlled. Forexample, the profile curve length of a half of the entrance pupildiameter (HEP) of the object-side surface of the first lens is denotedby ARE11, the thickness of the first lens on the optical axis is TP1,and the ratio between these two parameters is ARE11/TP1; the profilecurve length of a half of the entrance pupil diameter (HEP) of theimage-side surface of the first lens is denoted by ARE12, and the ratiobetween ARE12 and TP1 is ARE12/TP1. The profile curve length of a halfof the entrance pupil diameter (HEP) of the object-side surface of thesecond lens is denoted by ARE21, the thickness of the second lens on theoptical axis is TP2, and the ratio between these two parameters isARE21/TP2; the profile curve length of a half of the entrance pupildiameter (HEP) of the image-side surface of the second lens is denotedby ARE22, and the ratio between ARE22 and TP2 is ARE22/TP2. For anysurface of other lenses in the optical image capturing system, the ratiobetween the profile curve length of a half of the entrance pupildiameter (HEP) thereof and the thickness of the lens which the surfacebelonged to is denoted in the same manner.

In an embodiment, a height of the optical image capturing system (HOS)can be reduced while |f1|>f5.

In an embodiment, when |f2|+|f3|+|f4| and |f1|+|f5| of the lensessatisfy the aforementioned conditions, at least one lens among thesecond to the fourth lenses could have weak positive refractive power orweak negative refractive power. Herein the weak refractive power meansthe absolute value of the focal length of one specific lens is greaterthan 10. When at least one lens among the second to the fourth lenseshas weak positive refractive power, it may share the positive refractivepower of the first lens, and on the contrary, when at least one lensamong the second to the fourth lenses has weak negative refractivepower, it may fine turn and correct the aberration of the system.

In an embodiment, the fifth lens could have negative refractive power,and an image-side surface thereof is concave, it may reduce back focallength and size. Besides, the fifth lens can have at least an inflectionpoint on at least a surface thereof, which may reduce an incident angleof the light of an off-axis field of view and correct the aberration ofthe off-axis field of view.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

The present invention will be best understood by referring to thefollowing detailed description of some illustrative embodiments inconjunction with the accompanying drawings, in which

FIG. 1A is a schematic diagram of a first embodiment of the presentinvention;

FIG. 1B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the first embodiment of thepresent application;

FIG. 1C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the first embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 1D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the first embodiment of the present invention;

FIG. 1E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the first embodiment of the present disclosure;

FIG. 2A is a schematic diagram of a second embodiment of the presentinvention;

FIG. 2B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the second embodiment of thepresent application;

FIG. 2C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the second embodiment of the present application,and a transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 2D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the second embodiment of the present invention;

FIG. 2E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the second embodiment of the presentdisclosure;

FIG. 3A is a schematic diagram of a third embodiment of the presentinvention;

FIG. 3B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the third embodiment of thepresent application;

FIG. 3C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the third embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 3D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the third embodiment of the present invention;

FIG. 3E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the third embodiment of the present disclosure;

FIG. 4A is a schematic diagram of a fourth embodiment of the presentinvention;

FIG. 4B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the fourth embodiment of thepresent application;

FIG. 4C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the fourth embodiment of the present application,and a transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 4D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the fourth embodiment of the present invention;

FIG. 4E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the fourth embodiment of the presentdisclosure;

FIG. 5A is a schematic diagram of a fifth embodiment of the presentinvention;

FIG. 5B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the fifth embodiment of thepresent application;

FIG. 5C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the fifth embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 5D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the fifth embodiment of the present invention;

FIG. 5E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the fifth embodiment of the present disclosure;

FIG. 6A is a schematic diagram of a sixth embodiment of the presentinvention;

FIG. 6B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the sixth embodiment of thepresent application;

FIG. 6C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the sixth embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 6D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the sixth embodiment of the present invention; and

FIG. 6E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the sixth embodiment of the present disclosure.

DETAILED DESCRIPTION OF THE INVENTION

An optical image capturing system of the present invention includes afirst lens, a second lens, a third lens, a fourth lens, a fifth lens,and an image plane from an object side to an image side. The opticalimage capturing system further is provided with an image sensor at animage plane.

The optical image capturing system can work in three wavelengths,including 486, nm, 587.5 nm, and 656.2 nm, wherein 587.5 nm is the mainreference wavelength and is the reference wavelength for obtaining thetechnical characters. The optical image capturing system can also workin five wavelengths, including 470 nm, 510 nm, 555 nm, 610 nm, and 650nm wherein 555 nm is the main reference wavelength, and is the referencewavelength for obtaining the technical characters.

The optical image capturing system of the present invention satisfies0.5≤ΣPPR/|ΣNPR|≤3.0, and a preferable range is 1≤ΣPPR/|ΣNPR|≤2.5, wherePPR is a ratio of the focal length fp of the optical image capturingsystem to a focal length fp of each of lenses with positive refractivepower; NPR is a ratio of the focal length fn of the optical imagecapturing system to a focal length fn of each of lenses with negativerefractive power; ΣPPR is a sum of the PPRs of each positive lens; andΣNPR is a sum of the NPRs of each negative lens. It is helpful forcontrol of an entire refractive power and an entire length of theoptical image capturing system.

The image sensor is provided on the image plane. The optical imagecapturing system of the present invention satisfies HOS/HOI≤25 and0.5≤HOS/f≤25, and a preferable range is 1≤HOS/HOI≤20 and 1≤HOS/f≤20,where HOI is a half of a diagonal of an effective sensing area of theimage sensor, i.e., the maximum image height, and HOS is a height of theoptical image capturing system, i.e. a distance on the optical axisbetween the object-side surface of the first lens and the image plane.It is helpful for reduction of the size of the system for used incompact cameras.

The optical image capturing system of the present invention further isprovided with an aperture to increase image quality.

In the optical image capturing system of the present invention, theaperture could be a front aperture or a middle aperture, wherein thefront aperture is provided between the object and the first lens, andthe middle is provided between the first lens and the image plane. Thefront aperture provides a long distance between an exit pupil of thesystem and the image plane, which allows more elements to be installed.The middle could enlarge a view angle of view of the system and increasethe efficiency of the image sensor. The optical image capturing systemsatisfies 0.2≤InS/HOS≤1.1, where InS is a distance between the apertureand the image plane. It is helpful for size reduction and wide angle.

The optical image capturing system of the present invention satisfies0.1≤ΣTP/InTL≤0.9, where InTL is a distance between the object-sidesurface of the first lens and the image-side surface of the fifth lens,and ΣTP is a sum of central thicknesses of the lenses on the opticalaxis. It is helpful for the contrast of image and yield rate ofmanufacture and provides a suitable back focal length for installationof other elements.

The optical image capturing system of the present invention satisfies0.01<|R1/R2|<100, and a preferable range is 0.05<|R1/R2|<80, where R1 isa radius of curvature of the object-side surface of the first lens, andR2 is a radius of curvature of the image-side surface of the first lens.It provides the first lens with a suitable positive refractive power toreduce the increase rate of the spherical aberration.

The optical image capturing system of the present invention satisfies−50<(R9−R10)/(R9+R10)<50, where R9 is a radius of curvature of theobject-side surface of the fifth lens, and R10 is a radius of curvatureof the image-side surface of the fifth lens. It may modify theastigmatic field curvature.

The optical image capturing system of the present invention satisfiesIN12/f≤5.0, where IN12 is a distance on the optical axis between thefirst lens and the second lens. It may correct chromatic aberration andimprove the performance.

The optical image capturing system of the present invention satisfiesIN45/f≤55.0, where IN45 is a distance on the optical axis between thefourth lens and the fifth lens. It may correct chromatic aberration andimprove the performance.

The optical image capturing system of the present invention satisfies0.1≤(TP1+IN12)/TP≤50.0, where TP is a central thickness of the firstlens on the optical axis, and TP2 is a central thickness of the secondlens on the optical axis. It may control the sensitivity of manufactureof the system and improve the performance.

The optical image capturing system of the present invention satisfies0.1≤(TP5+IN45)/TP4≤50.0, where TP4 is a central thickness of the fourthlens on the optical axis, TP5 is a central thickness of the fifth lenson the optical axis, and IN45 is a distance between the fourth lens andthe fifth lens. It may control the sensitivity of manufacture of thesystem and improve the performance.

The optical image capturing system of the present invention satisfies0.1≤TP3/(IN23+TP3+IN34)<1, where TP2 is a central thickness of thesecond lens on the optical axis, TP3 is a central thickness of the thirdlens on the optical axis, TP4 is a central thickness of the fourth lenson the optical axis, IN23 is a distance on the optical axis between thesecond lens and the third lens, IN34 is a distance on the optical axisbetween the third lens and the fourth lens, and InTL is a distancebetween the object-side surface of the first lens and the image-sidesurface of the fifth lens. It may fine tune and correct the aberrationof the incident rays layer by layer, and reduce the height of thesystem.

The optical image capturing system satisfies 0 mm≤HVT51≤3 mm; 0mm<HVT52≤6 mm; 0≤HVT51/HVT52; 0 mm≤|SGC51|≤0.5 mm; 0 mm<|SGC52|≤2 mm;and 0<|SGC52|/(|SGC52|+TP5)≤0.9, where HVT51 a distance perpendicular tothe optical axis between the critical point C51 on the object-sidesurface of the fifth lens and the optical axis; HVT52 a distanceperpendicular to the optical axis between the critical point C52 on theimage-side surface of the fifth lens and the optical axis; SGC51 is adistance on the optical axis between a point on the object-side surfaceof the fifth lens where the optical axis passes through and a pointwhere the critical point C51 projects on the optical axis; SGC52 is adistance on the optical axis between a point on the image-side surfaceof the fifth lens where the optical axis passes through and a pointwhere the critical point C52 projects on the optical axis. It is helpfulto correct the off-axis view field aberration.

The optical image capturing system satisfies 0.2≤HVT52/HOI≤0.9, andpreferably satisfies 0.35≤HVT52/HOI≤0.8. It may help to correct theperipheral aberration.

The optical image capturing system satisfies 0≤HVT52/HOS≤0.5, andpreferably satisfies 0.2≤HVT52/HOS≤0.45. It may help to correct theperipheral aberration.

The optical image capturing system of the present invention satisfies0<SGI511(SGI511+TP5)≤0.9; 0<SGI521/(SGI521+TP5)≤0.9, and it ispreferable to satisfy 0.1≤SGI511/(SGI511+TP5)≤0.6;0.1≤SGI521/(SGI521+TP5)≤0.6, where SGI511 is a displacement on theoptical axis from a point on the object-side surface of the fifth lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the closest to the opticalaxis, projects on the optical axis, and SGI521 is a displacement on theoptical axis from a point on the image-side surface of the fifth lens,through which the optical axis passes, to a point where the inflectionpoint on the image-side surface, which is the closest to the opticalaxis, projects on the optical axis.

The optical image capturing system of the present invention satisfies0<SGI512/(SGI512+TP5)≤0.9; 0<SGI522/(SGI522+TP5)≤0.9, and it ispreferable to satisfy 0.1≤SGI512/(SGI512+TP5)≤0.6;0.1≤SGI522/(SGI522+TP5)≤0.6, where SGI512 is a displacement on theoptical axis from a point on the object-side surface of the fifth lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the second closest to theoptical axis, projects on the optical axis, and SGI522 is a displacementon the optical axis from a point on the image-side surface of the fifthlens, through which the optical axis passes, to a point where theinflection point on the image-side surface, which is the second closestto the optical axis, projects on the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF511|≤55 mm; 0.001 mm≤|HIF521|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF511|≤3.5 mm; 1.5 mm≤|HIF521|≤3.5 mm, where HIF511 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens, which is the closestto the optical axis, and the optical axis; HIF521 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the fifth lens, which is the closest to theoptical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF512|≤5 mm; 0.001 mm≤|HIF522|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF522|≤3.5 mm; 0.1 mm≤|HIF512|≤3.5 mm, where HIF512 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens, which is the secondclosest to the optical axis, and the optical axis; HIF522 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the fifth lens, which is the second closest to theoptical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF513|≤5 mm; 0.001 mm≤|HIF523|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF523|≤3.5 mm; 0.1 mm≤|HIF513|≤3.5 mm, where HIF513 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens, which is the thirdclosest to the optical axis, and the optical axis; HIF523 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the fifth lens, which is the third closest to theoptical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF514|≤5 mm; 0.001 mm≤|HIF524|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF524|≤3.5 mm; 0.1 mm≤|HIF514|≤3.5 mm, where HIF514 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens, which is the fourthclosest to the optical axis, and the optical axis; HIF524 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the fifth lens, which is the fourth closest to theoptical axis, and the optical axis.

In an embodiment, the lenses of high Abbe number and the lenses of lowAbbe number are arranged in an interlaced arrangement that could behelpful for correction of aberration of the system.

An equation of aspheric surface isz=ch²/[1+[1(k+1)ch²h²]^(0.5)]+A4h⁴+A6h⁶+A8h⁸+A10h¹⁰+A12h¹²+A14h¹⁴+A16h¹⁶+A18h¹⁸+A20h²⁰+. . . (1), where z is a depression of the aspheric surface; k is conicconstant; c is reciprocal of the radius of curvature; and A4, A6, A8,A10, A12, A14, A16, A18, and A20 are high-order aspheric coefficients.

In the optical image capturing system, the lenses could be made ofplastic or glass. The plastic lenses may reduce the weight and lower thecost of the system, and the glass lenses may control the thermal effectand enlarge the space for arrangement of the refractive power of thesystem. In addition, the opposite surfaces (object-side surface andimage-side surface) of the first to the fifth lenses could be asphericthat can obtain more control parameters to reduce aberration. The numberof aspheric glass lenses could be less than the conventional sphericalglass lenses, which is helpful for reduction of the height of thesystem.

When the lens has a convex surface, which means that the surface isconvex around a position, through which the optical axis passes, andwhen the lens has a concave surface, which means that the surface isconcave around a position, through which the optical axis passes.

The optical image capturing system of the present invention could beapplied in a dynamic focusing optical system. It is superior in thecorrection of aberration and high imaging quality so that it could beallied in lots of fields.

The optical image capturing system of the present invention couldfurther include a driving module to meet different demands, wherein thedriving module can be coupled with the lenses to move the lenses. Thedriving module can be a voice coil motor (VCM), which is used to movethe lens for focusing, or can be an optical image stabilization (OIS)component, which is used to lower the possibility of having the problemof image blurring which is caused by subtle movements of the lens whileshooting.

To meet different requirements, at least one lens among the first lensto the fifth lens of the optical image capturing system of the presentinvention can be a light filter, which filters out light of wavelengthshorter than 500 nm. Such effect can be achieved by coating on at leastone surface of the lens, or by using materials capable of filtering outshort waves to make the lens.

To meet different requirements, the image plane of the optical imagecapturing system in the present invention can be either flat or curved.If the image plane is curved (e.g., a sphere with a radius ofcurvature), the incidence angle required for focusing light on the imageplane can be decreased, which is not only helpful to shorten the lengthof the system (TTL), but also helpful to increase the relativeilluminance.

We provide several embodiments in conjunction with the accompanyingdrawings for the best understanding, which are:

First Embodiment

As shown in FIG. 1A and FIG. 1B, an optical image capturing system 10 ofthe first embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 110, an aperture100, a second lens 120, a third lens 130, a fourth lens 140, a fifthlens 150, an infrared rays filter 170, an image plane 180, and an imagesensor 190. FIG. 1C shows a tangential fan and a sagittal fan of theoptical image capturing system 10 of the first embodiment of the presentapplication, and a transverse aberration diagram at 0.7 field of viewwhen a longest operation wavelength and a shortest operation wavelengthpass through an edge of the aperture 100. FIG. 1D is a diagram showingthe through-focus MTF values of the visible light spectrum at thecentral field of view, 0.3 field of view, and 0.7 field of view of thefirst embodiment of the present invention. FIG. 1E is a diagram showingthe through-focus MTF values of the infrared light spectrum at thecentral field of view, 0.3 field of view, and 0.7 field of view of thefirst embodiment of the present disclosure.

The first lens 110 has negative refractive power and is made of plastic.An object-side surface 112 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 114 thereof, whichfaces the image side, is a concave aspheric surface. The object-sidesurface 112 has an inflection point thereon. A profile curve length ofthe maximum effective half diameter of an object-side surface of thefirst lens 110 is denoted by ARS11, and a profile curve length of themaximum effective half diameter of the image-side surface of the firstlens 110 is denoted by ARS12. A profile curve length of a half of anentrance pupil diameter (HEP) of the object-side surface of the firstlens 110 is denoted by ARE11, and a profile curve length of a half ofthe entrance pupil diameter (HEP) of the image-side surface of the firstlens 110 is denoted by ARE12. A thickness of the first lens 110 on theoptical axis is TP1.

The first lens satisfies SGI111=1.96546 mm;|SGI111|/(|SGI111|+TP1)=0.72369, where SGI111 is a displacement on theoptical axis from a point on the object-side surface of the first lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the closest to the opticalaxis, projects on the optical axis, and SGI121 is a displacement on theoptical axis from a point on the image-side surface of the first lens,through which the optical axis passes, to a point where the inflectionpoint on the image-side surface, which is the closest to the opticalaxis, projects on the optical axis.

The first lens satisfies HIF111=3.38542 mm; HIF111/HOI=0.90519, whereHIF111 is a displacement perpendicular to the optical axis from a pointon the object-side surface of the first lens, through which the opticalaxis passes, to the inflection point, which is the closest to theoptical axis; HIF121 is a displacement perpendicular to the optical axisfrom a point on the image-side surface of the first lens, through whichthe optical axis passes, to the inflection point, which is the closestto the optical axis.

The second lens 120 has positive refractive power and is made ofplastic. An object-side surface 122 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 124thereof, which faces the image side, is a concave aspheric surface. Aprofile curve length of the maximum effective half diameter of anobject-side surface of the second lens 120 is denoted by ARS21, and aprofile curve length of the maximum effective half diameter of theimage-side surface of the second lens 120 is denoted by ARS22. A profilecurve length of a half of an entrance pupil diameter (HEP) of theobject-side surface of the second lens 120 is denoted by ARE21, and aprofile curve length of a half of the entrance pupil diameter (HEP) ofthe image-side surface of the second lens 120 is denoted by ARE22. Athickness of the second lens 120 on the optical axis is TP2.

For the second lens, a displacement on the optical axis from a point onthe object-side surface of the second lens, through which the opticalaxis passes, to a point where the inflection point on the image-sidesurface, which is the closest to the optical axis, projects on theoptical axis, is denoted by SGI211, and a displacement on the opticalaxis from a point on the image-side surface of the second lens, throughwhich the optical axis passes, to a point where the inflection point onthe image-side surface, which is the closest to the optical axis,projects on the optical axis is denoted by SGI221.

For the second lens, a displacement perpendicular to the optical axisfrom a point on the object-side surface of the second lens, throughwhich the optical axis passes, to the inflection point, which is theclosest to the optical axis is denoted by HIF211, and a displacementperpendicular to the optical axis from a point on the image-side surfaceof the second lens, through which the optical axis passes, to theinflection point, which is the closest to the optical axis is denoted byHIF221.

The third lens 130 has positive refractive power and is made of plastic.An object-side surface 132, which faces the object side, is a convexaspheric surface, and an image-side surface 134, which faces the imageside, is a convex aspheric surface. The object-side surface 132 has aninflection point. A profile curve length of the maximum effective halfdiameter of an object-side surface of the third lens 130 is denoted byARS31, and a profile curve length of the maximum effective half diameterof the image-side surface of the third lens 130 is denoted by ARS32. Aprofile curve length of a half of an entrance pupil diameter (HEP) ofthe object-side surface of the third lens 130 is denoted by ARE31, and aprofile curve length of a half of the entrance pupil diameter (HEP) ofthe image-side surface of the third lens 130 is denoted by ARE32. Athickness of the third lens 130 on the optical axis is TP3.

The third lens 130 satisfies SGI311=0.00388 mm;|SGI311|/(ISGI311+TP3)=0.00414, where SGI311 is a displacement on theoptical axis from a point on the object-side surface of the third lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the closest to the opticalaxis, projects on the optical axis, and SGI321 is a displacement on theoptical axis from a point on the image-side surface of the third lens,through which the optical axis passes, to a point where the inflectionpoint on the image-side surface, which is the closest to the opticalaxis, projects on the optical axis.

For the third lens 130, SGI312 is a displacement on the optical axisfrom a point on the object-side surface of the third lens, through whichthe optical axis passes, to a point where the inflection point on theobject-side surface, which is the second closest to the optical axis,projects on the optical axis, and SGI322 is a displacement on theoptical axis from a point on the image-side surface of the third lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the second closest to theoptical axis, projects on the optical axis.

The third lens 130 further satisfies HIF311=0.38898 mm;HIF311/HOI=0.10400, where HIF311 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe third lens, which is the closest to the optical axis, and theoptical axis; HIF321 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the thirdlens, which is the closest to the optical axis, and the optical axis.

For the third lens 130, HIF312 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe third lens, which is the second closest to the optical axis, and theoptical axis; HIF322 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the thirdlens, which is the second closest to the optical axis, and the opticalaxis.

The fourth lens 140 has positive refractive power and is made ofplastic. An object-side surface 142, which faces the object side, is aconvex aspheric surface, and an image-side surface 144, which faces theimage side, is a convex aspheric surface. The object-side surface 142has an inflection point. A profile curve length of the maximum effectivehalf diameter of an object-side surface of the fourth lens 140 isdenoted by ARS41, and a profile curve length of the maximum effectivehalf diameter of the image-side surface of the fourth lens 140 isdenoted by ARS42. A profile curve length of a half of an entrance pupildiameter (HEP) of the object-side surface of the fourth lens 140 isdenoted by ARE41, and a profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the fourth lens 140 isdenoted by ARE42. A thickness of the fourth lens 140 on the optical axisis TP4.

The fourth lens 140 satisfies SGI421=0.06508 mm;|SGI421|/(|SGI421|+TP4)=0.03459, where SGI411 is a displacement on theoptical axis from a point on the object-side surface of the fourth lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the closest to the opticalaxis, projects on the optical axis, and SGI421 is a displacement on theoptical axis from a point on the image-side surface of the fourth lens,through which the optical axis passes, to a point where the inflectionpoint on the image-side surface, which is the closest to the opticalaxis, projects on the optical axis.

For the fourth lens 140, SGI412 is a displacement on the optical axisfrom a point on the object-side surface of the fourth lens, throughwhich the optical axis passes, to a point where the inflection point onthe object-side surface, which is the second closest to the opticalaxis, projects on the optical axis, and SGI422 is a displacement on theoptical axis from a point on the image-side surface of the fourth lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the second closest to theoptical axis, projects on the optical axis.

The fourth lens 140 further satisfies HIF421=0.85606 mm;HIF421/HOI=0.22889, where HIF411 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fourth lens, which is the closest to the optical axis, and theoptical axis; HIF421 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fourthlens, which is the closest to the optical axis, and the optical axis.

For the fourth lens 140, HIF412 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fourth lens, which is the second closest to the optical axis, andthe optical axis; HIF422 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fourthlens, which is the second closest to the optical axis, and the opticalaxis.

The fifth lens 150 has negative refractive power and is made of plastic.An object-side surface 152, which faces the object side, is a concaveaspheric surface, and an image-side surface 154, which faces the imageside, is a concave aspheric surface. The object-side surface 152 and theimage-side surface 154 both have an inflection point. A profile curvelength of the maximum effective half diameter of an object-side surfaceof the fifth lens 150 is denoted by ARS51, and a profile curve length ofthe maximum effective half diameter of the image-side surface of thefifth lens 150 is denoted by ARS52. A profile curve length of a half ofan entrance pupil diameter (HEP) of the object-side surface of the fifthlens 150 is denoted by ARE51, and a profile curve length of a half ofthe entrance pupil diameter (HEP) of the image-side surface of the fifthlens 150 is denoted by ARE52. A thickness of the fifth lens 150 on theoptical axis is TP5.

The fifth lens 150 satisfies SGI511=−1.51505 mm;|SGI511|/(|SGI511|+TP5)=0.70144; SGI521=0.01229 mm;|SGI521|(|SGI521|+TP5)=0.01870, where SGI511 is a displacement on theoptical axis from a point on the object-side surface of the fifth lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the closest to the opticalaxis, projects on the optical axis, and SGI521 is a displacement on theoptical axis from a point on the image-side surface of the fifth lens,through which the optical axis passes, to a point where the inflectionpoint on the image-side surface, which is the closest to the opticalaxis, projects on the optical axis.

For the fifth lens 150, SGI512 is a displacement on the optical axisfrom a point on the object-side surface of the fifth lens, through whichthe optical axis passes, to a point where the inflection point on theobject-side surface, which is the second closest to the optical axis,projects on the optical axis, and SGI522 is a displacement on theoptical axis from a point on the image-side surface of the fifth lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the second closest to theoptical axis, projects on the optical axis.

The fifth lens 150 further satisfies HIF511=2.25435 mm;HIF511/HOI=0.60277; HIF521=0.82313 mm; HIF521/HOI=0.22009, where HIF511is a distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens, which is the closestto the optical axis, and the optical axis; HIF521 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the fifth lens, which is the closest to theoptical axis, and the optical axis.

For the fifth lens 150, HIF512 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fifth lens, which is the second closest to the optical axis, and theoptical axis; HIF522 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fifthlens, which is the second closest to the optical axis, and the opticalaxis.

The infrared rays filter 170 is made of glass and between the fifth lens150 and the image plane 180. The infrared rays filter 170 gives nocontribution to the focal length of the system.

The optical image capturing system 10 of the first embodiment has thefollowing parameters, which are f=3.03968 mm; f/HEP=1.6; HAF=50.001; andtan(HAF)=1.1918, where f is a focal length of the system; HAF is a halfof the maximum field angle; and HEP is an entrance pupil diameter.

The parameters of the lenses of the first embodiment are f1=−9.24529 mm;|f/f1|=0.32878; f5=−2.32439; and |f1|>f5, where f1 is a focal length ofthe first lens 110; and f5 is a focal length of the fifth lens 150.

The first embodiment further satisfies |f2|+|f3|+|f4|=17.3009 mm;|f1|+|f5|=11.5697 mm and |f2|+|f3|+|f4|>|f1|+|f5|, where f2 is a focallength of the second lens 120, f3 is a focal length of the third lens130, f4 is a focal length of the fourth lens 140, and f5 is a focallength of the fifth lens 150.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣPPR=f/f2+f/f3+f/f4=1.86768; ΣNPR=f/f1+f/f5=−1.63651;ΣPPR/Σ|NPR|=1.14125; |f/f2|=0.47958; 1f/f3|=0.38289; |f/f4|=1.00521;|f/f5|=1.30773, where PPR is a ratio of a focal length fp of the opticalimage capturing system to a focal length fp of each of the lenses withpositive refractive power; and NPR is a ratio of a focal length fn ofthe optical image capturing system to a focal length fn of each oflenses with negative refractive power.

The optical image capturing system 10 of the first embodiment furthersatisfies InTL+BFL=HOS; HOS=10.56320 mm; HOI=3.7400 mm; HOS/HOI=2.8244;HOS/f=3.4751; InS=6.21073 mm; and InS/HOS=0.5880, where InTL is adistance between the object-side surface 112 of the first lens 110 andthe image-side surface 154 of the fifth lens 150; HOS is a height of theimage capturing system, i.e. a distance between the object-side surface112 of the first lens 110 and the image plane 180; InS is a distancebetween the aperture 100 and the image plane 180; HOI is a half of adiagonal of an effective sensing area of the image sensor 190, i.e., themaximum image height; and BFL is a distance between the image-sidesurface 154 of the fifth lens 150 and the image plane 180.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣTP=5.0393 mm; InTL=9.8514 mm and ΣTP/InTL=0.5115, where ΣTPis a sum of the thicknesses of the lenses 110-150 with refractive power.It is helpful for the contrast of image and yield rate of manufactureand provides a suitable back focal length for installation of otherelements.

The optical image capturing system 10 of the first embodiment furthersatisfies |R1/R2|=1.9672, where R1 is a radius of curvature of theobject-side surface 112 of the first lens 110, and R2 is a radius ofcurvature of the image-side surface 114 of the first lens 110. Itprovides the first lens with a suitable positive refractive power toreduce the increase rate of the spherical aberration.

The optical image capturing system 10 of the first embodiment furthersatisfies (R9−R10)/(R9+R10)=−1.1505, where R9 is a radius of curvatureof the object-side surface 152 of the fifth lens 150, and R10 is aradius of curvature of the image-side surface 154 of the fifth lens 150.It may modify the astigmatic field curvature.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣPP=f2+f3+f4=17.30090 mm; and f2/(f2+f3+f4)=0.36635, where ΣPPis a sum of the focal length fp of each lens with positive refractivepower. It is helpful to share the positive refractive power of thesecond lens 120 to other positive lenses to avoid the significantaberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣNP=f1+f5=−11.56968 mm; and f5/(f1+f5)=0.20090, where ΣNP is asum of the focal length fn of each lens with negative refractive power.It is helpful to share the negative refractive power of the fifth lens150 to the other negative lens, which avoids the significant aberrationcaused by the incident rays.

The optical image capturing system 10 of the first embodiment furthersatisfies IN12=3.19016 mm; IN12/f=1.04951, where IN12 is a distance onthe optical axis between the first lens 110 and the second lens 120. Itmay correct chromatic aberration and improve the performance.

The optical image capturing system 10 of the first embodiment furthersatisfies IN45=0.40470 mm; IN45/f=0.13314, where IN45 is a distance onthe optical axis between the fourth lens 140 and the fifth lens 150. Itmay correct chromatic aberration and improve the performance.

The optical image capturing system 10 of the first embodiment furthersatisfies TP1=0.75043 mm; TP2=0.89543 mm; TP3=0.93225 mm; and(TP1+IN12)/TP2=4.40078, where TP1 is a central thickness of the firstlens 110 on the optical axis, TP2 is a central thickness of the secondlens 120 on the optical axis, and TP3 is a central thickness of thethird lens 130 on the optical axis. It may control the sensitivity ofmanufacture of the system and improve the performance.

The optical image capturing system 10 of the first embodiment furthersatisfies TP4=1.81634 mm; TP5=0.64488 mm; and (TP5+IN45)/TP4=0.57785,where TP4 is a central thickness of the fourth lens 140 on the opticalaxis, TP5 is a central thickness of the fifth lens 150 on the opticalaxis, and IN45 is a distance on the optical axis between the fourth lens140 and the fifth lens 150. It may control the sensitivity ofmanufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment furthersatisfies TP2/TP3=0.96051; TP3/TP4=0.51325; TP4/TP5=2.81657; andTP3/(IN23+TP3+IN34)=0.43372, where IN34 is a distance on the opticalaxis between the third lens 130 and the fourth lens 140. It may controlthe sensitivity of manufacture of the system and lower the total heightof the system.

The optical image capturing system 10 of the first embodiment furthersatisfies InRS41=−0.09737 mm; InRS42=−1.31040 mm; |InRS4|/TP4=0.05361and |InRS42|/TP4=0.72145, where InRS41 is a displacement from a point onthe object-side surface 142 of the fourth lens 140 passed through by theoptical axis to a point on the optical axis where a projection of themaximum effective semi diameter of the object-side surface 142 of thefourth lens 140 ends; InRS42 is a displacement from a point on theimage-side surface 144 of the fourth lens 140 passed through by theoptical axis to a point on the optical axis where a projection of themaximum effective semi diameter of the image-side surface 144 of thefourth lens 140 ends; and TP4 is a central thickness of the fourth lens140 on the optical axis. It is helpful for manufacturing and shaping ofthe lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment furthersatisfies HVT41=1.41740 mm; HVT42=0, where HVT41 is a distanceperpendicular to the optical axis between the critical point on theobject-side surface 142 of the fourth lens and the optical axis; andHVT42 is a distance perpendicular to the optical axis between thecritical point on the image-side surface 144 of the fourth lens and theoptical axis.

The optical image capturing system 10 of the first embodiment furthersatisfies InRS51=−1.63543 mm; InRS52=−0.34495 mm; |InRS51|/TP5=2.53604and |InRS52|/TP5=0.53491, where InRS51 is a displacement from a point onthe object-side surface 152 of the fifth lens 150 passed through by theoptical axis to a point on the optical axis where a projection of themaximum effective semi diameter of the object-side surface 152 of thefifth lens 150 ends; InRS52 is a displacement from a point on theimage-side surface 154 of the fifth lens 150 passed through by theoptical axis to a point on the optical axis where a projection of themaximum effective semi diameter of the image-side surface 154 of thefifth lens 150 ends; and TP5 is a central thickness of the fifth lens150 on the optical axis. It is helpful for manufacturing and shaping ofthe lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment satisfiesHVT51=0; HVT52=1.35891 mm; and HVT51/HVT52=0, where HVT51 a distanceperpendicular to the optical axis between the critical point on theobject-side surface 152 of the fifth lens and the optical axis; andHVT52 a distance perpendicular to the optical axis between the criticalpoint on the image-side surface 154 of the fifth lens and the opticalaxis.

The optical image capturing system 10 of the first embodiment satisfiesHVT52/HOI=0.36334. It is helpful for correction of the aberration of theperipheral view field of the optical image capturing system.

The optical image capturing system 10 of the first embodiment satisfiesHVT52/HOS=0.12865. It is helpful for correction of the aberration of theperipheral view field of the optical image capturing system.

The third lens 130 and the fifth lens 150 have negative refractivepower. The optical image capturing system 10 of the first embodimentfurther satisfies NA5/NA3=0.368966, where NA3 is an Abbe number of thethird lens 130; and NA5 is an Abbe number of the fifth lens 150. It maycorrect the aberration of the optical image capturing system.

The optical image capturing system 10 of the first embodiment furthersatisfies |TDT|=0.63350%; |ODT|=2.06135%, where TDT is TV distortion;and ODT is optical distortion.

In the present embodiment, the lights of any field of view can befurther divided into sagittal ray and tangential ray, and the spatialfrequency of 220 cycles/mm serves as the benchmark for assessing thefocus shifts and the values of MTF. The focus shifts where thethrough-focus MTF values of the visible sagittal ray at the centralfield of view, 0.3 field of view, and 0.7 field of view of the opticalimage capturing system are at their respective maxima are denoted byVSFS0, VSFS3, and VSFS7 (unit of measurement: mm), respectively. Thevalues of VSFS0, VSFS3, and VSFS7 equal to 0.000 mm, 0.000 mm, and−0.020 mm, respectively. The maximum values of the through-focus MTF ofthe visible sagittal ray at the central field of view, 0.3 field ofview, and 0.7 field of view are denoted by VSMTF0, VSMTF3, and VSMTF7,respectively. The values of VSMTF0, VSMTF3, and VSMTF7 equal to 0.383,0.352, and 0.304, respectively. The focus shifts where the through-focusMTF values of the visible tangential ray at the central field of view,0.3 field of view, and 0.7 field of view of the optical image capturingsystem are at their respective maxima, are denoted by VTFS0, VTFS3, andVTFS7 (unit of measurement: mm), respectively. The values of VTFS0,VTFS3, and VTFS7 equal to 0.000 mm, 0.030 mm, and 0.010 mm,respectively. The maximum values of the through-focus MTF of the visibletangential ray at the central field of view, 0.3 field of view, and 0.7field of view are denoted by VTMTF0, VTMTF3, and VTMTF7, respectively.The values of VTMTF0, VTMTF3, and VTMTF7 equal to 0.383, 0.311, and0.179, respectively. The average focus shift (position) of both theaforementioned focus shifts of the visible sagittal ray at three fieldsof view and focus shifts of the visible tangential ray at three fieldsof view is denoted by AVFS (unit of measurement: mm), which satisfiesthe absolute value |(VSFS0+VSFS3+VSFS7+VTFS0+VTFS3+VTFS7)/6|=|0.003 mm|.

The focus shifts where the through-focus MTF values of the infraredsagittal ray at the central field of view, 0.3 field of view, and 0.7field of view of the optical image capturing system are at theirrespective maxima, are denoted by ISFS0, ISFS3, and ISFS7 (unit ofmeasurement: mm), respectively. The values of ISFS0, ISFS3, and ISFS7equal to 0.060 mm, 0.060 mm, and 0.030 mm, respectively. The averagefocus shift (position) of the aforementioned focus shifts of theinfrared sagittal ray at three fields of view is denoted by AISFS (unitof measurement: mm). The maximum values of the through-focus MTF of theinfrared sagittal ray at the central field of view, 0.3 field of view,and 0.7 field of view are denoted by ISMTF0, ISMTF3, and ISMTF7,respectively. The values of ISMTF0, ISMTF3, and ISMTF7 equal to 0.642,0.653, and 0.254, respectively. The focus shifts where the through-focusMTF values of the infrared tangential ray at the central field of view,0.3 field of view, and 0.7 field of view of the optical image capturingsystem are at their respective maxima, are denoted by ITFS0, ITFS3, andITFS7 (unit of measurement: mm), respectively. The values of ITFS0.ITFS3, and ITFS7 equal to 0.060, 0.070, and 0.030, respectively. Theaverage focus shift (position) of the aforementioned focus shifts of theinfrared tangential ray at three fields of view is denoted by AITFS(unit of measurement: mm). The maximum values of the through-focus MTFof the infrared tangential ray at the central field of view, 0.3 fieldof view, and 0.7 field of view are denoted by ITMTF0, ITMTF3, andITMTF7, respectively. The values of ITMTF0, ITMTF3, and ITMTF7 equal to0.642, 0.446, and 0.239, respectively. The average focus shift(position) of both of the aforementioned focus shifts of the infraredsagittal ray at the three fields of view and focus shifts of theinfrared tangential ray at the three fields of view is denoted by AIFS(unit of measurement: mm), which equals to the absolute value of|(ISFS0+ISFS3+ISFS7+ITFS0+ITFS3+ITFS7)/6|=10.052 mm|.

The focus shift (difference) between the focal points of the visiblelight and the infrared light at their central fields of view (RGB/IR) ofthe entire optical image capturing system (i.e. wavelength of 850 nmversus wavelength of 555 nm, unit of measurement: mm) is denoted by FS(the distance between the first and second image planes on the opticalaxis), which satisfies the absolute value|(VSFS0+VTFS0)/2−(ISFS0+ITFS0)/2|=|0.060 mm|. The difference (focusshift) between the average focus shift of the visible light in the threefields of view and the average focus shift of the infrared light in thethree fields of view (RGB/IR) of the entire optical image capturingsystem is denoted by AFS (i.e. wavelength of 850 nm versus wavelength of555 nm, unit of measurement: mm), for which the absolute value of|AIFS−AVFS|=|0.048 mm| is satisfied.

For the fifth lens 150 of the optical image capturing system 10 in thefirst embodiment, a transverse aberration at 0.7 field of view in thepositive direction of the tangential fan after the longest operationwavelength passing through the edge of the aperture 100 is denoted byPLTA, and is −0.042 mm; a transverse aberration at 0.7 field of view inthe positive direction of the tangential fan after the shortestoperation wavelength passing through the edge of the aperture 100 isdenoted by PSTA, and is 0.056 mm; a transverse aberration at 0.7 fieldof view in the negative direction of the tangential fan after thelongest operation wavelength passing through the edge of the aperture100 is denoted by NLTA, and is −0.011 mm; a transverse aberration at 0.7field of view in the negative direction of the tangential fan after theshortest operation wavelength passing through the edge of the aperture100 is denoted by NSTA, and is −0.024 mm; a transverse aberration at 0.7field of view of the sagittal fan after the longest operation wavelengthpassing through the edge of the aperture 100 is denoted by SLTA, and is−0.013 mm; a transverse aberration at 0.7 field of view of the sagittalfan after the shortest operation wavelength passing through the edge ofthe aperture 100 is denoted by SSTA, and is 0.018 mm.

The parameters of the lenses of the first embodiment are listed in Table1

TABLE 1 f = 3.03968 mm; f/HEP = 1.6; HAF = 50.0010 deg Radius ofcurvature Thickness Refractive Abbe Focal length Surface (mm) (mm)Material index number (mm) 0 Object plane infinity 1 1^(st) lens4.01438621 0.750 plastic 1.514 56.80 −9.24529 2 2.040696375 3.602 3Aperture plane −0.412 4 2^(nd) lens 2.45222384 0.895 plastic 1.565 58.006.33819 5 6.705898264 0.561 6 3^(rd) lens 16.39663088 0.932 plastic1.565 58.00 7.93877 7 −6.073735083 0.656 8 4^(th) lens 4.421363446 1.816plastic 1.565 58.00 3.02394 9 −2.382933539 0.405 10 5^(th) lens−1.646639396 0.645 plastic 1.650 21.40 −2.32439 11 23.53222697 0.100 12Infrared rays plane 0.200 BK7_SCH 1.517 64.20 filter 13 plane 0.412 14Image plane plane Reference wavelength: 555 nm.

TABLE 2 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k−1.882119E−01  −1.927558E+00  −6.483417E+00  1.766123E+01 −5.000000E+01−3.544648E+01  −3.167522E+01 A4 7.686381E−04 3.070422E−02 5.439775E−027.241691E−03 −2.985209E−02 −6.315366E−02  −1.903506E−03 A6 4.630306E−04−3.565153E−03  −7.980567E−03  −8.359563E−03  −7.175713E−03 6.038040E−03−1.806837E−03 A8 3.178966E−05 2.062259E−03 −3.537039E−04  1.303430E−02 4.284107E−03 4.674156E−03 −1.670351E−03 A10 −1.773597E−05 −1.571117E−04  2.844845E−03 −6.951350E−03  −5.492349E−03 −8.031117E−03  4.791024E−04 A12 1.620619E−06 −4.694004E−05  −1.025049E−03 1.366262E−03  1.232072E−03 3.319791E−03 −5.594125E−05 A14 −4.916041E−08 7.399980E−06 1.913679E−04 3.588298E−04 −4.107269E−04 −5.356799E−04  3.704401E−07 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 A18 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00 A200.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+000.000000E+00  0.000000E+00 Surface 9 10 11 k −2.470764E+00 −1.570351E+00 4.928899E+01 A4 −2.346908E−04  −4.250059E−04−4.625703E−03  A6 2.481207E−03 −1.591781E−04 −7.108872E−04  A8−5.862277E−04  −3.752177E−05 3.429244E−05 A10 −1.955029E−04 −9.210114E−05 2.887298E−06 A12 1.880941E−05 −1.101797E−05 3.684628E−07A14 1.132586E−06  3.536320E−06 −4.741322E−08  A16 0.000000E+00 0.000000E+00 0.000000E+00 A18 0.000000E+00  0.000000E+00 0.000000E+00A20 0.000000E+00  0.000000E+00 0.000000E+00

The figures related to the profile curve lengths obtained based on Table1 and Table 2 are listed in the following table:

First embodiment (Reference wavelength: 555 nm) ARE ARE − 2(ARE/ ARE/TPARE 1/2(HEP) value 1/2(HEP) HEP) % TP (%) 11 0.950 0.958 0.008 100.87%0.750 127.69% 12 0.950 0.987 0.037 103.91% 0.750 131.53% 21 0.950 0.9760.026 102.74% 0.895 108.99% 22 0.950 0.954 0.004 100.42% 0.895 106.52%31 0.950 0.949 −0.001 99.94% 0.932 101.83% 32 0.950 0.959 0.009 100.93%0.932 102.84% 41 0.950 0.953 0.003 100.29% 1.816 52.45% 42 0.950 0.9700.020 102.15% 1.816 53.42% 51 0.950 0.995 0.045 104.71% 0.645 154.24% 520.950 0.949 −0.001 99.92% 0.645 147.18% ARS ARS − (ARS/ ARS/TP ARS EHDvalue EHD EHD)% TP (%) 11 3.459 4.210 0.751 121.71% 0.750 561.03% 122.319 3.483 1.165 150.24% 0.750 464.19% 21 1.301 1.384 0.084 106.43%0.895 154.61% 22 1.293 1.317 0.024 101.87% 0.895 147.09% 31 1.400 1.4470.047 103.39% 0.932 155.22% 32 1.677 1.962 0.285 116.97% 0.932 210.45%41 2.040 2.097 0.057 102.82% 1.816 115.48% 42 2.338 2.821 0.483 120.67%1.816 155.32% 51 2.331 2.971 0.639 127.43% 0.645 460.64% 52 3.219 3.2670.049 101.51% 0.645 506.66%

The detail parameters of the first embodiment are listed in Table 1, inwhich the unit of the radius of curvature, thickness, and focal lengthare millimeter, and surface 0-10 indicates the surfaces of all elementsin the system in sequence from the object side to the image side. Table2 is the list of coefficients of the aspheric surfaces, in which A1-A20indicate the coefficients of aspheric surfaces from the first order tothe twentieth order of each aspheric surface. The following embodimentshave the similar diagrams and tables, which are the same as those of thefirst embodiment, so we do not describe it again.

Second Embodiment

As shown in FIG. 2A and FIG. 2B, an optical image capturing system 20 ofthe second embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 210, asecond lens 220, an aperture 200, a third lens 230, a fourth lens 240, afifth lens 250, an infrared rays filter 270, an image plane 280, and animage sensor 290. FIG. 2C shows a tangential fan and a sagittal fan ofthe optical image capturing system of the second embodiment of thepresent application, and a transverse aberration diagram at 0.7 field ofview when a longest operation wavelength and a shortest operationwavelength pass through an edge of the aperture. FIG. 2D is a diagramshowing the through-focus MTF values of the visible light spectrum atthe central field of view, 0.3 field of view, and 0.7 field of view ofthe second embodiment of the present invention. FIG. 2E is a diagramshowing the through-focus MTF values of the infrared light spectrum atthe central field of view, 0.3 field of view, and 0.7 field of view ofthe second embodiment of the present disclosure.

The first lens 210 has positive refractive power and is made of plastic.An object-side surface 212 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 214 thereof, whichfaces the image side, is a concave aspheric surface. The object-sidesurface 212 and the image-side surface 214 both have an inflectionpoint.

The second lens 220 has negative refractive power and is made ofplastic. An object-side surface 222 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 224thereof, which faces the image side, is a concave aspheric surface. Theobject-side surface 222 and the image-side surface 224 both have aninflection point.

The third lens 230 has positive refractive power and is made of plastic.An object-side surface 232, which faces the object side, is a convexaspheric surface, and an image-side surface 234, which faces the imageside, is a convex aspheric surface. The object-side surface 232 has twoinflection points and the image-side surface 234 has an inflectionpoint.

The fourth lens 240 has negative refractive power and is made ofplastic. An object-side surface 242, which faces the object side, is aconcave aspheric surface, and an image-side surface 244, which faces theimage side, is a convex aspheric surface. The object-side surface 242and the image-side surface 244 both have two inflection points.

The fifth lens 250 has positive refractive power and is made of plastic.An object-side surface 252, which faces the object side, is a convexaspheric surface, and an image-side surface 254, which faces the imageside, is a concave aspheric surface. The object-side surface 252 and theimage-side surface 254 both have two inflection points. It may help toshorten the back focal length to keep small in size. In addition, it mayreduce an incident angle of the light of an off-axis field of view andcorrect the aberration of the off-axis field of view.

The infrared rays filter 270 is made of glass and between the fifth lens250 and the image plane 280. The infrared rays filter 270 gives nocontribution to the focal length of the system.

The parameters of the lenses of the second embodiment are listed inTable 3 and Table 4.

TABLE 3 f = 2.2578 mm; f/HEP = 1.8; HAF = 45 deg Radius of curvatureThickness Retractive Abbe Focal length Surface (mm) (mm) Material indexnumber (mm) 0 Object 1E+18 1E+18 1 Aperture 1E+18 −0.149 2 1^(st) lens1.277207602 0.371 plastic 1.544 56.064 2.600 3 10.91455102 0.032 42^(nd) lens 7.657328829 0.175 plastic 1.661 20.381 −6.195 5 2.6852557570.195 6 3^(rd) lens 10.38856573 0.359 plastic 1.584 29.878 2.426 7−1.650527875 0.127 8 4^(th) lens −0.751875136 0.245 plastic 1.661 20.381−1.548 9 −3.010174736 0.136 10 5^(th) lens 0.702443378 0.696 plastic1.544 56.064 2.130 11 1.141958508 0.316 12 Infrared rays 1E+18 0.150NBK7 1.517 64.135 filter 13 1E+18 0.396 14 Image plane 1E+18 0.000Reference wavelength: 555 nm; the position of blocking light: theeffective half diameter of the clear aperture of the seventh surface is0.725 mm.

TABLE 4 Coefficients of the aspheric surfaces Surface 2 3 4 5 6 7 8 k6.179690E−18 9.801626E−16 1.115336E−16 6.280409E−17 −2.093062E−16 5.277586E−17 −6.096340E−01  A4 −7.251812E−02  −6.892532E−01 −8.262254E−01  −6.412526E−01  −7.533309E−01 −5.856730E−01 4.142116E−01A6 1.564906E−01 2.970160E+00 3.869164E+00 3.355642E+00  1.708275E+00−4.753064E+00 −7.146733E+00  A8 −2.599357E−01  1.385347E+00−1.315145E+00  −1.353686E+01  −2.178572E+01  2.419303E+01 5.424177E+01A10 −3.594268E+00  −6.293952E+01  −4.903277E+01  4.432966E+01 8.778744E+01 −3.684063E+01 −1.557410E+02  A12 2.542908E+01 2.145003E+021.408229E+02 −1.372112E+02  −1.485136E+02 −4.003736E+00 2.202255E+02 A14−7.259780E+01  −3.266423E+02  −1.483159E+02  2.541525E+02  1.342011E+02 8.379568E+01 −1.517251E+02  A16 6.652350E+01 2.023735E+02 5.227631E+01−1.834302E+02  −6.282913E+01 −7.159193E+01 3.905064E+01 A18 2.425248E+000.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+000.000000E+00 Surface 9 10 11 k −8.756919E+01 −6.892288E+00−1.366878E+00  A4 −1.628248E+00 −1.468941E−01 −2.582747E−01  A6 6.665330E+00 −5.017966E−02 2.138568E−02 A8 −1.227311E+01  2.677063E−011.460555E−01 A10  1.232626E+01 −3.118483E−01 −1.438475E−01  A12−6.842035E+00  1.654456E−01 6.171812E−02 A14  1.885483E+00 −4.125520E−02−1.305912E−02  A16 −1.817675E−01  3.947747E−03 1.108572E−03 A18 0.000000E+00  0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the second embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the second embodiment based on Table 3 and Table4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f1/f2| 0.11902 0.21413 0.26886 0.44686 0.50404 1.79909ΣPPR ΣNPR ΣPPR/ IN12/f IN45/f |f2/f3| |ΣNPR| 0.6610 0.8919 0.7411 2.28320.0170 1.2556 TP3/(IN23 + TP3 + IN34) (TP1 + IN12)/TP2 (TP5 + IN45)/TP40.36813 1.32852 0.87835 HOS InTL HOS/HOI InS/HOS ODT % TDT % 49.5777044.83540 12.39443 0.40576 −123.983 108.351 HVT41 HVT42 HVT51 HVT52HVT52/ HVT52/ HOI HOS 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000TP2/TP3 TP3/TP4 InRS51 InRS52 |InRS51|/ |InRS52|/ TP5 TP5 0.757142.28094 −1.33349 0.589597 0.41596 0.18392 PSTA PLTA NSTA NLTA SSTA SLTA−0.005 0.010 mm −0.006 mm 0.016 mm 0.016 mm 0.001 mm mm VSFS0 VSFS3VSFS7 VTFS0 VTFS3 VTFS7 −0.000 −0.000 0.005 −0.000 −0.010 −0.000 VSMTF0VSMTF3 VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.742 0.754 0.713 0.742 0.638 0.744ISFS0 ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 −0.010 −0.010 0.005 −0.010 −0.0100.025 ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.870 0.883 0.739 0.8700.869 0.654 FS AIFS AVFS AFS 0.010 −0.002 −0.001 0.001

The figures related to the profile curve lengths obtained based on Table3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) ARE ARE − 2(ARE/ ARE/TPARE 1/2(HEP) value 1/2(HEP) HEP) % TP (%) 11 0.815 0.814 −0.00085 99.90%1.807 45.06% 12 0.815 0.815 −0.00019 99.98% 1.807 45.09% 21 0.815 0.814−0.00087 99.89% 6.401 12.72% 22 0.815 0.815 0.00063 100.08% 6.401 12.74%31 0.815 0.815 −0.00028 99.97% 8.455 9.63% 32 0.815 0.815 0.00016100.02% 8.455 9.64% 41 0.815 0.815 0.00027 100.03% 3.707 21.99% 42 0.8150.817 0.00213 100.26% 3.707 22.04% 51 0.815 0.817 0.00220 100.27% 3.20625.49% 52 0.815 0.814 −0.00055 99.93% 3.206 25.40% ARS ARS − (ARS/ARS/TP ARS EHD value EHD EHD)% TP (%) 11 17.665 17.880 0.216 101.22%1.807 989.67% 12 11.636 13.116 1.481 112.72% 1.807 725.97% 21 10.12310.128 0.005 100.05% 6.401 158.21% 22 5.404 6.206 0.802 114.84% 6.40196.94% 31 3.070 3.095 0.025 100.81% 8.455 36.60% 32 4.530 4.763 0.234105.16% 8.455 56.34% 41 4.503 4.614 0.111 102.46% 3.707 124.47% 42 4.4354.729 0.294 106.62% 3.707 127.57% 51 4.322 4.546 0.224 105.18% 3.206141.81% 52 3.648 3.702 0.054 101.49% 3.206 115.47%

The results of the equations of the second embodiment based on Table 3and Table 4 are listed in the following table:

Values related to the inflection points of the second embodiment(Reference wavelength: 555 nm) HIF111 0.5704 HIF111/HOI 0.2480 SGI1110.126744 |SGI111|/(|SGI111| + TP1) 0.2546 HIF121 0.1134 HIF121/HOI0.0493 SGI121 0.0005 |SGI121|/(|SGI121| + TP1) 0.0013 HIF211 0.1272HIF211/HOI 0.0553 SGI211 0.0008568 |SGI211|/(|SGI211| + TP2) 0.0049HIF221 0.3998 HIF221/HOI 0.1738 SGI221 0.0214 |SGI221|/(|SGI221| + TP2)0.1087 HIF311 0.1058 HIF311/HOI 0.0460 SGI311 0.0004|SGI311|/(|SGI311| + TP3) 0.0012 HIF312 0.5500 HIF312/HOI 0.2391 SGI312−0.0542 |SGI312|/(|SGI312| + TP3) 0.1311 HIF321 0.5432 HIF321/HOI 0.2362SGI321 −0.1545 |SGI321|/(|SGI321| + TP3) 0.3007 HIF411 0.4284 HIF411/HOI0.1863 SGI411 −0.119915 |SGI411|/(|SGI411| + TP4) 0.3290 HIF412 0.7178HIF412/HOI 0.3121 SGI412 −0.2286 |SGI412|/(|SGI412| + TP4) 0.4832 HIF4210.4421 HIF421/HOI 0.1922 SGI421 −0.0513 |SGI421|/(|SGI421| + TP4) 0.1734HIF422 0.8052 HIF422/HOI 0.3501 SGI422 −0.1060 |SGI422|/(|SGI422| + TP4)0.3023 HIF511 0.4043 HIF511/HOI 0.1758 SGI511 0.0816363|SGI511|/(|SGI511| + TP5) 0.1050 HIF512 1.3374 HIF512/HOI 0.5815 SGI5120.1332 |SGI512|/(|SGI512| + TP5) 0.1607 HIF521 0.5660 HIF521/HOI 0.2461SGI521 0.1125 |SGI521|/(|SGI521| + TP5) 0.1393 HIF522 1.7616 HIF522/HOI0.7659 SGI522 −0.0929 |SGI522|/(|SGI522| + TP5) 0.1178

Third Embodiment

As shown in FIG. 3A and FIG. 3B, an optical image capturing system ofthe third embodiment of the present invention includes, along an opticalaxis from an object side to an image side, an aperture 300, a first lens310, a second lens 320, a third lens 330, a fourth lens 340, a fifthlens 350, an infrared rays filter 370, an image plane 380, and an imagesensor 390. FIG. 3C shows a tangential fan and a sagittal fan of theoptical image capturing system of the third embodiment of the presentapplication, and a transverse aberration diagram at 0.7 field of viewwhen a longest operation wavelength and a shortest operation wavelengthpass through an edge of the aperture. FIG. 3D is a diagram showing thethrough-focus MTF values of the visible light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the thirdembodiment of the present invention. FIG. 3E is a diagram showing thethrough-focus MTF values of the infrared light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the thirdembodiment of the present disclosure.

The first lens 310 has positive refractive power and is made of plastic.An object-side surface 312 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 314 thereof, whichfaces the image side, is a concave aspheric surface.

The second lens 320 has negative refractive power and is made ofplastic. An object-side surface 322 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 324thereof, which faces the image side, is a concave aspheric surface. Theobject-side surface 322 has an inflection point.

The third lens 330 has positive refractive power and is made of plastic.An object-side surface 332 thereof, which faces the object side, is aconcave aspheric surface, and an image-side surface 334 thereof, whichfaces the image side, is a convex aspheric surface. The object-sidesurface 332 and the image-side surface 334 both have an inflectionpoint.

The fourth lens 340 has negative refractive power and is made ofplastic. An object-side surface 342, which faces the object side, is aconcave aspheric surface, and an image-side surface 344, which faces theimage side, is a convex aspheric surface. The object-side surface 342and the image-side surface 344 both have two inflection points.

The fifth lens 350 has positive refractive power and is made of plastic.An object-side surface 352, which faces the object side, is a convexaspheric surface, and an image-side surface 354, which faces the imageside, is a concave aspheric surface. The object-side surface 352 and theimage-side surface 354 both have two inflection points. It may help toshorten the back focal length to keep small in size.

The infrared rays filter 370 is made of glass and between the fifth lens350 and the image plane 380. The infrared rays filter 370 gives nocontribution to the focal length of the system.

The parameters of the lenses of the third embodiment are listed in Table5 and Table 6.

TABLE 5 f = 2.6916 mm; f/HEP = 2.2; HAF = 40.0072 deg Radius ofcurvature Thickness Refractive Abbe Focal length Surface (mm) (mm)Material index number (mm) 0 Object 1E+18 1E+18 1 Aperture 1E+18 −0.2002 1^(st) lens 1.054490795 0.331 plastic 1.544 56.064 2.395 3 4.7344996560.091 4 2^(nd) lens 32.92014849 0.150 plastic 1.661 20.381 −8.239 54.762237826 0.252 6 3^(rd) lens −4.534356197 0.390 plastic 1.584 29.8783.877 7 −1.57545536 0.095 8 4^(th) lens −0.809338874 0.275 plastic 1.66120.381 −1.586 9 −3.735517644 0.101 10 5^(th) lens 0.670106861 0.626plastic 1.544 56.064 2.177 11 1.020745086 0.250 12 Infrared rays 1E+180.150 BK_7 1.517 64.13 filter 13 1E+18 0.718 14 Image plane 1E+18 0.000Reference wavelength: 555 nm; the position of blocking light: no.

TABLE 6 Coefficients of the aspheric surfaces Surface 2 3 4 5 6 7 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+005.277586E−17 −6.329528E−01  A4 1.041629E−02 −9.437109E−02 −1.790879E−01  −2.944867E−01  −7.263328E−01  3.165429E−01 2.106241E+00A6 2.342363E−01 −9.946261E−01  −1.236484E+00  1.375950E+00 1.244539E+00−1.049673E+01  −1.792849E+01  A8 −7.755000E−01  1.225317E+011.501271E+01 −6.445474E+00  −1.915800E+01  4.359374E+01 8.100256E+01 A10−2.079589E+00  −7.043099E+01  −6.215127E+01  4.076140E+01 8.484921E+01−8.308689E+01  −1.890488E+02  A12 2.542908E+01 2.145003E+02 1.408229E+02−1.372112E+02  −1.490887E+02  8.445120E+01 2.432787E+02 A14−7.259781E+01  −3.266423E+02  −1.483159E+02  2.541525E+02 1.342011E+02−3.727437E+01  −1.651104E+02  A16 6.652350E+01 2.023735E+02 5.227631E+01−1.834302E+02  −6.282913E+01  1.998370E+00 4.621983E+01 A18 2.425248E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 k −8.756919E+01 −6.341332E+00−2.329042E+00  A4 −1.168847E+00 −5.235840E−01 −4.405883E−01  A6 4.252268E+00  8.281161E−01 4.144087E−01 A8 −7.634620E+00 −9.974292E−01−2.554309E−01  A10  8.184753E+00  7.337532E−01 7.058507E−02 A12−5.364832E+00 −3.123473E−01 3.073582E−03 A14  1.993328E+00  7.288994E−02−6.348393E−03  A16 −3.254001E−01 −7.310500E−03 1.044315E−03 A18 0.000000E+00  0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the third embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the third embodiment based on Table 5 and Table6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f1/f2| 1.12375 0.32667 0.69431 1.69722 1.23642 0.29070ΣPPR ΣNPR ΣPPR/ IN12/f IN45/f |f2/f3| |ΣNPR| 3.2603 1.8181 1.7933 0.03380.0375 2.1254 TP3/(IN23 + TP3 + IN34) (TP1 + IN12)/TP2 (TP5 + IN45)/TP40.52938 2.81511 2.64307 HOS InTL HOS/HOI InS/HOS ODT % TDT % 3.428892.31103 1.49082 0.94167 1.81039 2.01065 HVT41 HVT42 HVT51 HVT52HVT52/HOI HVT52/ HOS 0 0 0.80431 1.00062 0.34970 0.23457 TP2/TP3 TP3/TP4InRS51 InRS52 |InRS51|/ |InRS52|/ TP5 TP5 0.38451 1.41855 0.0209071−0.162758 0.03340 0.26005 PSTA PLTA NSTA NLTA SSTA SLTA 0.007 mm 0.025mm 0.005 mm 0.003 mm 0.021 mm 0.020 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3VTFS7 0.000 −0.009 0.003 0.000 0.000 −0.003 VSMTF0 VSMTF3 VSMTF7 VTMTF0VTMTF3 VTMTF7 0.808 0.726 0.573 0.808 0.583 0.504 ISFS0 ISFS3 ISFS7ITFS0 ITFS3 ITFS7 0.003 −0.006 0.012 0.003 0.012 0.021 ISMTF0 ISMTF3ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.734 0.583 0.597 0.734 0.495 0.467 FS AIFSAVFS AFS 0.003 0.008 −0.002 0.008

The figures related to the profile curve lengths obtained based on Table5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) ARE ARE − 2(ARE/ ARE/TPARE 1/2(HEP) value 1/2(HEP) HEP) % TP (%) 11 0.612 0.654 0.04204 106.87%0.331 197.40% 12 0.612 0.612 0.00014 100.02% 0.331 184.75% 21 0.6120.612 0.00005 100.01% 0.150 407.85% 22 0.612 0.617 0.00553 100.90% 0.150411.51% 31 0.612 0.632 0.02066 103.38% 0.390 162.11% 32 0.612 0.6530.04136 106.76% 0.390 167.42% 41 0.612 0.640 0.02803 104.58% 0.275232.64% 42 0.612 0.618 0.00605 100.99% 0.275 224.65% 51 0.612 0.6240.01275 102.08% 0.626 99.78% 52 0.612 0.625 0.01303 102.13% 0.626 99.82%ARS ARS − (ARS/ ARS/TP ARS EHD value EHD EHD)% TP (%) 11 0.612 0.6540.04204 106.87% 0.331 197.40% 12 0.619 0.619 0.00013 100.02% 0.331186.88% 21 0.630 0.631 0.00130 100.21% 0.150 420.98% 22 0.623 0.6300.00712 101.14% 0.150 419.98% 31 0.646 0.669 0.02285 103.54% 0.390171.37% 32 0.770 0.824 0.05401 107.01% 0.390 211.23% 41 0.851 0.8910.03946 104.63% 0.275 323.93% 42 1.138 1.154 0.01674 101.47% 0.275419.72% 51 1.468 1.495 0.02733 101.86% 0.626 238.89% 52 1.700 1.8330.13339 107.85% 0.626 292.91%

The results of the equations of the third embodiment based on Table 5and Table 6 are listed in the following table:

Values related to the inflection points of the third embodiment(Reference wavelength: 555 nm) HIF211 0.1105 HIF211/HOI 0.0480 SGI2110.000157 |SGI211|/(|SGI211| + TP2) 0.0010 HIF212 0.3857 HIF212/HOI0.1677 SGI212 −0.00165 |SGI212|/(|SGI212| + TP2) 0.0109 HIF311 0.5449HIF311/HOI 0.2369 SGI311 −0.0961 |SGI311|/(|SGI311| + TP3) 0.1976 HIF3210.5634 HIF321/HOI 0.2450 SGI321 −0.158715 |SGI321|/(|SGI321| + TP3)0.2892 HIF411 0.4782 HIF411/HOI 0.2079 SGI411 −0.117345|SGI411|/(|SGI411| + TP4) 0.2991 HIF412 0.7491 HIF412/HOI 0.3257 SGI412−0.2136 |SGI412|/(|SGI412| + TP4) 0.4372 HIF421 0.5024 HIF421/HOI 0.2184SGI421 −0.0559 |SGI421|/(|SGI421| + TP4) 0.1690 HIF422 0.8707 HIF422/HOI0.3786 SGI422 −0.1183 |SGI422|/(|SGI422| + TP4) 0.3007 HIF511 0.3239HIF511/HOI 0.1408 SGI511 0.0577 |SGI511|/(|SGI511| + TP5) 0.0844 HIF5121.1850 HIF512/HOI 0.5152 SGI512 0.0705 |SGI512|/(|SGI512| + TP5) 0.1012HIF521 0.4599 HIF521/HOI 0.2000 SGI521 0.0812 |SGI521|/(|SGI521| + TP5)0.1148 HIF522 1.5856 HIF522/HOI 0.6894 SGI522 −0.0947|SGI522|/(|SGI522| + TP5) 0.1315

Fourth Embodiment

As shown in FIG. 4A and FIG. 4B, an optical image capturing system 40 ofthe fourth embodiment of the present invention includes, along anoptical axis from an object side to an image side, an aperture 400, afirst lens 410, a second lens 420, a third lens 430, a fourth lens 440,a fifth lens 450, an infrared rays filter 470, an image plane 480, andan image sensor 490. FIG. 4C shows a tangential fan and a sagittal fanof the optical image capturing system of the fourth embodiment of thepresent application, and a transverse aberration diagram at 0.7 field ofview when a longest operation wavelength and a shortest operationwavelength pass through an edge of the aperture. FIG. 4D is a diagramshowing the through-focus MTF values of the visible light spectrum atthe central field of view, 0.3 field of view, and 0.7 field of view ofthe fourth embodiment of the present invention. FIG. 4E is a diagramshowing the through-focus MTF values of the infrared light spectrum atthe central field of view, 0.3 field of view, and 0.7 field of view ofthe fourth embodiment of the present disclosure.

The first lens 410 has positive refractive power and is made of plastic.An object-side surface 412 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 414 thereof, whichfaces the image side, is a convex aspheric surface. The object-sidesurface 412 has an inflection point.

The second lens 420 has negative refractive power and is made ofplastic. An object-side surface 422 thereof, which faces the objectside, is a concave aspheric surface, and an image-side surface 424thereof, which faces the image side, is a concave aspheric surface. Theobject-side surface 422 and the image-side surface 424 both have aninflection point.

The third lens 430 has negative refractive power and is made of plastic.An object-side surface 432 thereof, which faces the object side, is aconcave aspheric surface, and an image-side surface 434 thereof, whichfaces the image side, is a concave aspheric surface. The object-sidesurface 432 has an inflection point and the image-side surface 434 hastwo inflection points.

The fourth lens 440 has negative refractive power and is made ofplastic. An object-side surface 442, which faces the object side, is aconcave aspheric surface, and an image-side surface 444, which faces theimage side, is a convex aspheric surface. The object-side surface 442has two inflection points and the image-side surface 444 has fourinflection points.

The fifth lens 450 has positive refractive power and is made of plastic.An object-side surface 452, which faces the object side, is a convexaspheric surface, and an image-side surface 454, which faces the imageside, is a concave aspheric surface. The object-side surface 452 has twoinflection points and the image-side surface 454 has an inflectionpoint. It may help to shorten the back focal length to keep small insize.

The infrared rays filter 470 is made of glass and between the fifth lens450 and the image plane 480. The infrared rays filter 470 gives nocontribution to the focal length of the system.

The parameters of the lenses of the fourth embodiment are listed inTable 7 and Table 8.

TABLE 7 f = 2.6908 mm; f/HEP = 2.2; HAF = 40.0178 deg Radius ofcurvature Thickness Refractive Abbe Focal length Surface (mm) (mm)Material index number (mm) 0 Object 1E+18 1E+18 1 Aperture 1E+18 −0.1152 1^(st) lens 1.366169859 0.364 plastic 1.544 56.064 2.129 3−7.319634612 0.053 4 2^(nd) lens −6.020429771 0.175 plastic 1.661 20.381−6.556 5 17.11092475 0.281 6 3^(rd) lens −7.237264032 0.187 plastic1.661 20.381 −4.265 7 4.856730751 0.155 8 4^(th) lens −3.88228352 0.352plastic 1.584 29.878 −50.913 9 −4.604717727 0.158 10 5^(th) lens0.763066891 0.600 plastic 1.544 56.064 3.480 11 0.916490027 0.281 12Infrared rays 1E+18 0.150 BK_7 1.517 64.13 filter 13 1E+18 0.735 14Image plane 1E+18 0.000 Reference wavelength: 555 nm; the position ofblocking light: no.

TABLE 8 Coefficients of the aspheric surfaces Surface 7 3 4 5 6 7 8 k6.179690E−18 9.801626E−16 1.115336E−16 6.280409E−17 −2.093062E−165.277586E−17 2.391785E+00 A4 −8.925978E−02  2.304647E−01 5.566884E−015.212557E−02 −1.098357E+00 −5.035681E−01  7.057830E−01 A6 2.973447E−02−1.990299E+00  −2.381261E+00  7.493821E−01  1.754280E+00 1.358555E−01−4.020751E−02  A8 −5.282446E−01  1.181615E+01 1.288947E+01−7.717934E+00  −1.257984E+01 −3.449966E+00  −5.572540E+00  A10−4.033332E+00  −7.038182E+01  −5.845509E+01  4.175881E+01  6.100805E+011.368577E+01 1.463601E+01 A12 2.542908E+01 2.145003E+02 1.408229E+02−1.372112E+02  −1.263260E+02 −1.532295E+01  −1.777589E+01  A14−7.259781E+01  −3.266423E+02  −1.483159E+02  2.541525E+02  1.342011E+024.847043E+00 1.110904E+01 A16 6.652350E+01 2.023735E+02 5.227631E+01−1.834302E+02  −6.282913E+01 6.740200E−01 −2.938279E+00  A182.425248E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+000.000000E+00 0.000000E+00 Surface 9 10 11 k −8.753246E+01 −5.596357E+00−3.028644E+00 A4 −1.183477E+00 −4.151232E−01 −2.988790E−01 A6 5.345741E+00  6.844273E−01  2.683804E−01 A8 −1.150885E+01 −1.034066E+00−2.046910E−01 A10  1.364770E+01  8.667727E−01  9.652147E−02 A12−9.026138E+00 −3.829835E−01 −2.611804E−02 A14  3.120395E+00 8.587931E−02  3.593657E−03 A16 −4.421887E−01 −7.768617E−03−1.825391E−04 A18  0.000000E+00  0.000000E+00  0.000000E+00

An equation of the aspheric surfaces of the fourth embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the fourth embodiment based on Table 7 and Table8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f1/f2| 1.26384 0.41041 0.63088 0.05285 0.77325 0.32473ΣPPR ΣNPR ΣPPR/ IN12/f IN45/f |f2/f3| |ΣNPR| 1.2365 1.8947 0.6526 0.01950.0586 1.5372 TP3/(IN23 + TP3 + IN34) (TP1 + IN12)/TP2 (TP5 + IN45)/TP40.29970 2.38184 2.15590 HOS InTL HOS/HOI InS/HOS ODT % TDT % 3.490422.32394 1.51757 0.96710 1.80134 0.649573 HVT41 HVT42 HVT51 HVT52 HVT52/HVT52/HOS HOI 0.32677 0 0.81384 1.06460 0.35384 0.23316 TP2/TP3 TP3/TP4InRS51 InRS52 |InRS51|/ |InRS52|/ TP5 TP5 0.93763 0.53096 0.0310062−0.043063 0.05166 0.07175 PSTA PLTA NSTA NLTA SSTA SLTA −0.011 −0.001−0.006 −0.009 0.005 mm 0.003 mm mm mm mm mm VSFS0 VSFS3 VSFS7 VTFS0VTFS3 VTFS7 −0.000 −0.010 0.005 −0.000 −0.000 −0.000 VSMTF0 VSMTF3VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.804 0.754 0.637 0.804 0.627 0.571 ISFS0ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 0.005 −0.005 0.005 0.005 0.005 0.015ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.731 0.671 0.569 0.731 0.5950.516 FS AIFS AVFS AFS 0.005 0.005 −0.001 0.006

The figures related to the profile curve lengths obtained based on Table7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) ARE ARE − 2(ARE/ ARE/TPARE 1/2(HEP) value 1/2(HEP) HEP) % TP (%) 11 0.612 0.624 0.01261 102.06%0.364 171.36% 12 0.612 0.616 0.00448 100.73% 0.364 169.12% 21 0.6120.611 −0.00041 99.93% 0.175 349.22% 22 0.612 0.612 0.00070 100.11% 0.175349.86% 31 0.612 0.630 0.01867 103.05% 0.187 337.66% 32 0.612 0.6140.00218 100.36% 0.187 328.83% 41 0.612 0.611 −0.00009 99.98% 0.352173.95% 42 0.612 0.615 0.00386 100.63% 0.352 175.07% 51 0.612 0.6260.01405 102.30% 0.600 104.23% 52 0.612 0.630 0.01806 102.95% 0.600104.90% ARS ARS − (ARS/ ARS/TP ARS EHD value EHD EHD)% TP (%) 11 0.6120.624 0.01261 102.06% 0.364 171.36% 12 0.674 0.685 0.01078 101.60% 0.364187.93% 21 0.722 0.726 0.00413 100.57% 0.175 414.92% 22 0.713 0.7240.01117 101.57% 0.175 413.59% 31 0.742 0.764 0.02157 102.91% 0.187409.36% 32 0.801 0.805 0.00453 100.57% 0.187 431.34% 41 0.986 0.9880.00239 100.24% 0.352 281.05% 42 1.175 1.185 0.01046 100.89% 0.352337.24% 51 1.579 1.613 0.03363 102.13% 0.600 268.73% 52 1.826 1.9960.17000 109.31% 0.600 332.55%

The results of the equations of the fourth embodiment based on Table 7and Table 8 are listed in the following table:

Values related to the inflection points of the fourth embodiment(Reference wavelength: 555 nm) HIF111 0.4869 HIF111/HOI 0.2117 SGI1110.0825 |SGI111|/(|SGI111| + TP1) 0.1847 HIF211 0.1841 HIF211/HOI 0.0801SGI211 −0.0023 |SGI211|/(|SGI211| + TP2) 0.0127 HIF221 0.7061 HIF221/HOI0.3070 SGI221 0.0684 |SGI221|/(|SGI221| + TP2) 0.2810 HIF311 0.5446HIF311/HOI 0.2368 SGI311 −0.0913 |SGI311|/(|SGI311| + TP3) 0.3286 HIF3210.1842 HIF321/HOI 0.0801 SGI321 0.0029 |SGI321|/(|SGI321| + TP3) 0.0154HIF322 0.5972 HIF322/HOI 0.2596 SGI322 −0.0257 |SGI322|/(|SGI322| + TP3)0.1209 HIF411 0.1787 HIF411/HOI 0.0777 SGI411 −0.0034|SGI411|/(|SGI411| + TP4) 0.0096 HIF412 0.5498 HIF412/HOI 0.2390 SGI4120.0030 |SGI412|/(|SGI412| + TP4) 0.0084 HIF421 0.4633 HIF421/HOI 0.2014SGI421 −0.0404 |SGI421|/(|SGI421| + TP4) 0.1030 HIF422 0.6780 HIF422/HOI0.2948 SGI422 −0.0741 |SGI422|/(|SGI422| + TP4) 0.1742 HIF423 0.7601HIF423/HOI 0.3305 SGI423 −0.0863 |SGI423|/(|SGI423| + TP4) 0.1971 HIF4241.0190 HIF424/HOI 0.4430 SGI424 −0.1145 |SGI424|/(|SGI424| + TP4) 0.2457HIF511 0.3749 HIF511/HOI 0.1630 SGI511 0.0685 |SGI511|/(|SGI511| + TP5)0.1024 HIF512 1.1548 HIF512/HOI 0.5021 SGI512 0.0802|SGI512|/(|SGI512| + TP5) 0.1179 HIF521 0.4982 HIF521/HOI 0.2166 SGI5210.1046 |SGI521|/(|SGI521| + TP5) 0.1484

Fifth Embodiment

As shown in FIG. 5A and FIG. 5B, an optical image capturing system ofthe fifth embodiment of the present invention includes, along an opticalaxis from an object side to an image side, an aperture 500, a first lens510, a second lens 520, a third lens 530, a fourth lens 540, a fifthlens 550, an infrared rays filter 570, an image plane 580, and an imagesensor 590. FIG. 5C shows a tangential fan and a sagittal fan of theoptical image capturing system of the fifth embodiment of the presentapplication, and a transverse aberration diagram at 0.7 field of viewwhen a longest operation wavelength and a shortest operation wavelengthpass through an edge of the aperture. FIG. 5D is a diagram showing thethrough-focus MTF values of the visible light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the fifthembodiment of the present invention. FIG. 5E is a diagram showing thethrough-focus MTF values of the infrared light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the fifthembodiment of the present disclosure.

The first lens 510 has positive refractive power and is made of plastic.An object-side surface 512, which faces the object side, is a convexaspheric surface, and an image-side surface 514, which faces the imageside, is a convex aspheric surface. The image-side surface 514 has twoinflection points.

The second lens 520 has negative refractive power and is made ofplastic. An object-side surface 522 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 524thereof, which faces the image side, is a concave aspheric surface. Theobject-side surface 522 has an inflection point.

The third lens 530 has positive refractive power and is made of plastic.An object-side surface 532, which faces the object side, is a convexaspheric surface, and an image-side surface 534, which faces the imageside, is a convex aspheric surface. The object-side surface 532 and theimage-side surface 534 both have an inflection point.

The fourth lens 540 has positive refractive power and is made ofplastic. An object-side surface 542, which faces the object side, is aconcave aspheric surface, and an image-side surface 544, which faces theimage side, is a convex aspheric surface. The image-side surface 544 hasan inflection point.

The fifth lens 550 has negative refractive power and is made of plastic.An object-side surface 552, which faces the object side, is a convexaspheric surface, and an image-side surface 554, which faces the imageside, is a concave aspheric surface. The object-side surface 552 and theimage-side surface 554 both have two inflection points.

The infrared rays filter 570 is made of glass and between the fifth lens550 and the image plane 580. The infrared rays filter 570 gives nocontribution to the focal length of the system.

The parameters of the lenses of the fifth embodiment are listed in Table9 and Table 10.

TABLE 9 f = 2.6923 mm; f/HEP = 2.4; HAF = 40.0026 deg Radius ofcurvature Thickness Refractive Abbe Focal length Surface (mm) (mm)Material index number (mm) 0 Object 1E+18 1E+18 1 Aperture 1E+18 −0.1502 1^(st) lens 1.178647566 0.349 plastic 1.544 56.064 1.946 3 −10.20976730.025 4 2^(nd) lens 39.19187721 0.200 plastic 1.661 20.381 −2.856 51.839258376 0.201 6 3^(rd) lens 7.488606449 0.407 plastic 1.544 56.0649.900 7 −19.42817624 0.214 8 4^(th) lens −1.48740053 0.545 plastic 1.54456.064 1.703 9 −0.648697199 0.043 10 5^(th) lens 4.251001132 0.448plastic 1.544 56.064 −1.724 11 0.744987591 0.221 12 Infrared rays 1E+180.115 1.517 64.13 filter 13 1E+18 0.760 14 Image plane 1E+18 0.000Reference wavelength: 555 nm; the position of blocking light: no.

TABLE 10 Coefficients of the aspheric surfaces Surface 2 3 4 5 6 7 8 k−8.339571E−19  1.301450E−27 0.000000E+00 4.749688E−16 0.000000E+003.210355E−26 9.193610E−01 A4 3.210861E−02 5.329850E−01 3.926013E−01−6.839780E−02  −2.640126E−01  8.087066E−03 3.734776E−01 A6 1.999579E−01−2.735624E+00  −2.509260E+00  5.346538E−01 1.955041E−01 −1.657775E+00 −2.406666E+00  A8 −4.957039E−01  1.986917E+01 1.649499E+01−3.088719E+00  −3.363644E+00  1.009982E+01 1.201166E+01 A10 2.786807E−01−1.084454E+02  −8.163651E+01  9.364886E+00 1.524260E+01 −3.643918E+01 −2.852418E+01  A12 7.570721E+00 3.637850E+02 2.533409E+02 −2.149238E+00 −4.403523E+01  7.144109E+01 3.653006E+01 A14 −2.105392E+01 −6.525638E+02  −4.376949E+02  −4.205709E+01  6.728911E+01 −7.622623E+01 −2.580813E+01  A16 1.790538E+01 4.602319E+02 2.956021E+02 5.727823E+01−3.680918E+01  3.492594E+01 8.071808E+00 A18 2.425248E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface9 10 11 k −3.703092E+00 −2.123961E+01 −6.688536E+00  A4 −5.181981E−01−5.198737E−01 −2.647368E−01  A6  7.380653E−01  5.200410E−01 2.273446E−01A8 −7.399555E−01 −2.464770E−02 −1.339032E−01  A10  2.205173E+00−6.064853E−01 2.967215E−02 A12 −3.266108E+00  5.927428E−01 5.569599E−03A14  2.013430E+00 −2.198199E−01 −4.340542E−03  A16 −4.481287E−01 2.900498E−02 6.683326E−04 A18  0.000000E+00  0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the fifth embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the fifth embodiment based on Table 9 and Table10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f1/f2| 1.38333 0.94269 0.27194 1.58060 1.56186 0.68146ΣPPR ΣNPR ΣPPR/ IN12/f IN45/f |f2/f3| |ΣNPR| 4.0851 1.6553 2.4680 0.00930.0159 0.2885 TP3/(IN23 + TP3 + IN34) (TP1 + IN12)/TP2 (TP5 + IN45)/TP40.49487 1.87160 0.90029 HOS InTL HOS/HOI InS/HOS ODT % TDT % 3.529342.43298 1.53450 0.95746 1.80254 1.79768 HVT41 HVT42 HVT51 HVT52HVT52/HOI HVT52/ HOS 0 0 0.36084 0.94630 0.15689 0.10224 TP2/TP3 TP3/TP4InRS51 InRS52 |InRS51|/ |InRS52|/ TP5 TP5 0.49161 0.74582 −0.294611−0.236065 0.65713 0.52654 PSTA PLTA NSTA NLTA SSTA SLTA 0.006 mm 0.002mm 0.001 mm 0.006 mm 0.008 mm 0.005 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3VTFS7 0.001 −0.005 −0.005 0.001 0.001 −0.005 VSMTF0 VSMTF3 VSMTF7 VTMTF0VTMTF3 VTMTF7 0.808 0.789 0.692 0.808 0.749 0.599 ISFS0 ISFS3 ISFS7ITFS0 ITFS3 ITFS7 0.008 −0.000 −0.008 0.008 0.003 −0.005 ISMTF0 ISMTF3ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.701 0.689 0.619 0.701 0.670 0.507 FS AIFSAVFS AFS 0.007 0.001 −0.002 0.003

The figures related to the profile curve lengths obtained based on Table9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) ARE ARE − 2(ARE/ ARE/TPARE 1/2(HEP) value 1/2(HEP) HEP) % TP (%) 11 0.561 0.587 0.02599 104.63%0.349 168.01% 12 0.561 0.560 −0.00056 99.90% 0.349 160.40% 21 0.5610.560 −0.00057 99.90% 0.200 280.16% 22 0.561 0.569 0.00798 101.42% 0.200284.44% 31 0.561 0.561 −0.00007 99.99% 0.407 137.85% 32 0.561 0.5610.00008 100.01% 0.407 137.89% 41 0.561 0.570 0.00901 101.61% 0.545104.48% 42 0.561 0.606 0.04516 108.05% 0.545 111.10% 51 0.561 0.560−0.00048 99.92% 0.448 125.00% 52 0.561 0.574 0.01295 102.31% 0.448127.99% ARS ARS − (ARS/ ARS/TP ARS EHD value EHD EHD)% TP (%) 11 0.5610.588 0.02694 104.80% 0.349 168.34% 12 0.583 0.582 −0.00045 99.92% 0.349166.71% 21 0.588 0.588 0.00032 100.05% 0.200 294.17% 22 0.627 0.6400.01249 101.99% 0.200 319.95% 31 0.663 0.666 0.00323 100.49% 0.407163.69% 32 0.818 0.844 0.02661 103.25% 0.407 207.54% 41 0.878 0.9210.04252 104.84% 0.545 168.83% 42 1.084 1.187 0.10325 109.53% 0.545217.64% 51 1.273 1.339 0.06630 105.21% 0.448 298.70% 52 1.641 1.8070.16547 110.08% 0.448 403.01%

The results of the equations of the fifth embodiment based on Table 9and Table 10 are listed in the following table:

Values related to the inflection points of the fifth embodiment(Reference wavelength: 555 nm) HIF121 0.1375 HIF121/HOI 0.0598 SGI121−0.0008 |SGI121|/(|SGI121| + TP1) 0.0021 HIF122 0.5297 HIF122/HOI 0.2303SGI122 0.0082 |SGI122|/(|SGI122| + TP1) 0.0229 HIF211 0.4718 HIF211/HOI0.2051 SGI211 0.0112477 |SGI211|/(|SGI211| + TP2) 0.0532 HIF311 0.2054HIF311/HOI 0.0893 SGI311 0.002353 |SGI311|/(|SGI311| + TP3) 0.0058HIF321 0.7752 HIF321/HOI 0.3370 SGI321 −0.1096 |SGI321|/(|SGI321| + TP3)0.2123 HIF421 0.6139 HIF421/HOI 0.2669 SGI421 −0.2435|SGI421|/(|SGI421| + TP4) 0.3086 HIF511 0.1978 HIF511/HOI 0.0860 SGI5110.003789 |SGI511|/(|SGI511| + TP5) 0.0084 HIF512 1.1159 HIF512/HOI0.4852 SGI512 −0.2050 |SGI512|/(|SGI512| + TP5) 0.3138 HIF521 0.3820HIF521/HOI 0.1661 SGI521 0.0709 |SGI521|/(|SGI521| + TP5) 0.1366 HIF5221.6085 HIF522/HOI 0.6994 SGI522 −0.1948 |SGI522|/(|SGI522| + TP5) 0.3029

Sixth Embodiment

As shown in FIG. 6A and FIG. 6B, an optical image capturing system ofthe sixth embodiment of the present invention includes, along an opticalaxis from an object side to an image side, an aperture 600, a first lens610, a second lens 620, a third lens 630, a fourth lens 640, a fifthlens 650, an infrared rays filter 670, an image plane 680, and an imagesensor 690. FIG. 6C shows a tangential fan and a sagittal fan of theoptical image capturing system of the sixth embodiment of the presentapplication, and a transverse aberration diagram at 0.7 field of viewwhen a longest operation wavelength and a shortest operation wavelengthpass through an edge of the aperture. FIG. 6D is a diagram showing thethrough-focus MTF values of the visible light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the sixthembodiment of the present invention. FIG. 6E is a diagram showing thethrough-focus MTF values of the infrared light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the sixthembodiment of the present disclosure.

The first lens 610 has positive refractive power and is made of plastic.An object-side surface 612, which faces the object side, is a convexaspheric surface, and an image-side surface 614, which faces the imageside, is a convex aspheric surface. The object-side surface 612 has aninflection point.

The second lens 620 has negative refractive power and is made ofplastic. An object-side surface 622 thereof, which faces the objectside, is a concave aspheric surface, and an image-side surface 624thereof, which faces the image side, is a concave aspheric surface. Theobject-side surface 622 has an inflection point.

The third lens 630 has negative refractive power and is made of plastic.An object-side surface 632, which faces the object side, is a concaveaspheric surface, and an image-side surface 634, which faces the imageside, is a convex aspheric surface. The object-side surface 632 and theimage-side surface 634 both have an inflection point.

The fourth lens 640 has negative refractive power and is made ofplastic. An object-side surface 642, which faces the object side, is aconcave aspherical surface, and an image-side surface 644, which facesthe image side, is a convex aspherical surface. The object-side surface642 and the image-side surface 644 both have two inflection points.

The fifth lens 650 has positive refractive power and is made of plastic.An object-side surface 652, which faces the object side, is a convexaspherical surface, and an image-side surface 654, which faces the imageside, is a concave aspherical surface. The object-side surface 652 hastwo inflection points and the image-side surface 654 has an inflectionpoint. It may help to shorten the back focal length to keep small insize. In addition, it may reduce an incident angle of the light of anoff-axis field of view and correct the aberration of the off-axis fieldof view.

The infrared rays filter 670 is made of glass and between the fifth lens650 and the image plane 680. The infrared rays filter 670 gives nocontribution to the focal length of the system.

The parameters of the lenses of the sixth embodiment are listed in Table11 and Table 12.

TABLE 11 f = 2.6919 mm; f/HEP = 2.4; HAF = 40.0059 deg Radius ofcurvature Thickness Retractive Abbe Focal length Surface (mm) (mm)Material index number (mm) 0 Object 1E+18 1E+18 1 Aperture 1E+18 −0.1252 1^(st) lens 1.176338934 0.362 plastic 1.544 56.064 1.818 3−5.870931192 0.052 4 2^(nd) lens −4.263016305 0.175 plastic 1.661 20.381−3.914 5 7.124438312 0.278 6 3^(rd) lens −3.923367895 0.190 plastic1.661 20.381 −10.437 7 −8.991128003 0.140 8 4^(th) lens −1.9569176110.382 plastic 1.544 56.064 −14.449 9 −2.777445252 0.100 10 5^(th) lens0.940870596 0.694 plastic 1.544 56.064 5.258 11 1.031168418 0.281 12Infrared rays 1E+18 0.150 BK_7 1.517 64.13 filter 13 1E+18 0.620 14Image plane 1E+18 0.000 Reference wavelength: 555 nm; the position ofblocking light: no.

TABLE 12 Coefficients of the aspheric surfaces Surface 2 3 4 5 6 7 8 k 6.179690E−18 9.801626E−16 1.115336E−16 6.280409E−17 −2.093062E−165.277586E−17 5.066908E−01 A4 −5.065447E−02 2.105104E−01 6.527466E−013.136484E−01 −9.645838E−01 −6.083945E−01  7.405767E−01 A6 −1.461820E−01−2.150975E+00  −2.877184E+00  −1.242287E−01   1.910227E+00 1.420632E+00−5.140370E−01  A8 −2.510017E−03 1.312939E+01 1.564537E+01 −4.428156E+00 −1.751337E+01 −1.336940E+01  −6.123715E+00  A10 −5.437291E+00−7.246708E+01  −6.167159E+01  3.804736E+01  7.774187E+01 5.128667E+012.307335E+01 A12  2.542908E+01 2.145003E+02 1.408229E+02 −1.372112E+02 −1.423718E+02 −8.710724E+01  −3.592932E+01  A14 −7.259781E+01−3.266423E+02  −1.483159E+02  2.541525E+02  1.342011E+02 7.957155E+012.677580E+01 A16  6.652350E+01 2.023735E+02 5.227631E+01 −1.834302E+02 −6.282913E+01 −3.405060E+01  −7.875622E+00  A18  2.425248E+000.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 k −8.751949E+01 −7.762722E+00 −2.566412E+00A4 −1.327636E+00 −5.562941E−01 −3.710165E−01 A6  5.594825E+00 1.059041E+00  3.574232E−01 A8 −1.259829E+01 −1.584000E+00 −2.474820E−01A10  1.684221E+01  1.444010E+00  1.032455E−01 A12 −1.325389E+01−7.643446E−01 −2.466937E−02 A14  5.642259E+00  2.181854E−01 2.909277E−03 A16 −1.001651E+00 −2.590520E−02 −1.086081E−04 A18 0.000000E+00  0.000000E+00  0.000000E+00

An equation of the aspheric surfaces of the sixth embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the sixth embodiment based on Table 11 and Table12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f1/f2| 1.48033 0.68772 0.25792 0.18630 0.51200 0.46457ΣPPR ΣNPR ΣPPR/ IN12/f IN45/f |f2/f3| |ΣNPR| 1.4576 1.6666 0.8746 0.01930.0372 0.3750 TP3/(IN23 + TP3 + IN34) (TP1 + IN12)/TP2 (TP5 + IN45)/TP40.31210 2.36332 2.08100 HOS InTL HOS/HOI InS/HOS ODT % TDT % 3.423902.37216 1.48865 0.96351 1.80476 1.18323 HVT41 HVT42 HVT51 HVT52 HVT52/HVT52/ HOI HOS 0 0 0.73674 1.08264 0.32032 0.21518 TP2/TP3 TP3/TP4InRS51 InRS52 |InRS51|/ |InRS52|/ TP5 TP5 0.92221 0.49734 −0.055382−0.111752 0.07982 0.16106 PLTA PSTA NLTA NSTA SLTA SSTA 0.001 mm 0.002mm 0.002 mm 0.00037 mm 0.001 mm 0.001 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3VTFS7 −0.000 −0.010 −0.000 −0.000 −0.000 −0.005 VSMTF0 VSMTF3 VSMTF7VTMTF0 VTMTF3 VTMTF7 0.776 0.756 0.665 0.776 0.683 0.628 ISFS0 ISFS3ISFS7 ITFS0 ITFS3 ITFS7 −0.000 −0.015 −0.005 −0.000 −0.000 −0.000 ISMTF0ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.700 0.684 0.611 0.700 0.624 0.532FS AIFS AVFS AFS 0.000 −0.003 −0.003 0.001

The figures related to the profile curve lengths obtained based on Table11 and Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) ARE ARE − 2(ARE/ ARE/TPARE 1/2(HEP) value 1/2(HEP) HEP) % TP (%) 11 0.561 0.577 0.01651 102.94%0.362 159.61% 12 0.561 0.563 0.00194 100.35% 0.362 155.58% 21 0.5610.560 −0.00056 99.90% 0.175 320.15% 22 0.561 0.564 0.00315 100.56% 0.175322.26% 31 0.561 0.578 0.01716 103.06% 0.190 304.58% 32 0.561 0.5680.00717 101.28% 0.190 299.31% 41 0.561 0.562 0.00095 100.17% 0.382147.23% 42 0.561 0.567 0.00607 101.08% 0.382 148.57% 51 0.561 0.5670.00615 101.10% 0.694 81.71% 52 0.561 0.573 0.01193 102.13% 0.694 82.54%ARS ARS − (ARS/ ARS/TP ARS EHD value EHD EHD)% TP (%) 11 0.561 0.5770.01651 102.94% 0.362 159.61% 12 0.561 0.563 0.00194 100.35% 0.362155.58% 21 0.561 0.560 −0.00056 99.90% 0.175 320.15% 22 0.561 0.5640.00315 100.56% 0.175 322.26% 31 0.561 0.578 0.01716 103.06% 0.190304.58% 32 0.561 0.568 0.00717 101.28% 0.190 299.31% 41 0.561 0.5620.00095 100.17% 0.382 147.23% 42 0.561 0.567 0.00607 101.08% 0.382148.57% 51 0.561 0.567 0.00615 101.10% 0.694 81.71% 52 0.561 0.5730.01193 102.13% 0.694 82.54%

The results of the equations of the sixth embodiment based on Table 11and Table 12 are listed in the following table:

Values related to the inflection points of the sixth embodiment(Reference wavelength: 555 nm) HIF111 0.4896 HIF111/HOI 0.2129 SGI1110.0997 |SGI111|/(|SGI111| + TP1) 0.2161 HIF211 0.2105 HIF211/HOI 0.0915SGI211 −0.004119 |SGI211|/(|SGI211| + TP2) 0.0230 HIF311 0.5338HIF311/HOI 0.2321 SGI311 −0.098499 |SGI311|/(|SGI311| + TP3) 0.3417HIF321 0.5679 HIF321/HOI 0.2469 SGI321 −0.0724 |SGI321|/(|SGI321| + TP3)0.2761 HIF411 0.3031 HIF411/HOI 0.1318 SGI411 −0.0181|SGI411|/(|SGI411| + TP4) 0.0454 HIF412 0.3995 HIF412/HOI 0.1737 SGI412−0.0268 |SGI412|/(|SGI412| + TP4) 0.0656 HIF421 0.6094 HIF421/HOI 0.2650SGI421 −0.087702 |SGI421|/(|SGI421| + TP4) 0.1869 HIF422 0.8408HIF422/HOI 0.3656 SGI422 −0.142449 |SGI422|/(|SGI422| + TP4) 0.2718HIF511 0.3242 HIF511/HOI 0.1409 SGI511 0.0425873 |SGI511|/(|SGI511| +TP5) 0.0578 HIF512 1.2269 HIF512/HOI 0.5334 SGI512 −0.0223|SGI512|/(|SGI512| + TP5) 0.0311 HIF521 0.4907 HIF521/HOI 0.2133 SGI5210.0906321 |SGI521|/(|SGI521| + TP5) 0.1155

It must be pointed out that the embodiments described above are onlysome embodiments of the present invention. All equivalent structureswhich employ the concepts disclosed in this specification and theappended claims should fall within the scope of the present invention.

What is claimed is:
 1. An optical image capturing system, in order alongan optical axis from an object side to an image side, comprising: afirst lens having refractive power; a second lens having refractivepower; a third lens having refractive power; a fourth lens havingrefractive power; a fifth lens having positive refractive power; a firstimage plane, which is an image plane specifically for visible light andlocated at a position of the optical axis with a through-focusmodulation transfer rate (value of MTF) at a first spatial frequencyhaving a maximum value; and a second image plane, which is an imageplane specifically for infrared light and located at a position of theoptical axis with a through-focus modulation transfer rate (value ofMTF) at the first spatial frequency having a maximum value; wherein theoptical image capturing system has a total of the five lenses withrefractive power; at least one lens among the first lens to the fifthlens is made of plastic; at least one lens among the first lens to thefifth lens has positive refractive power; each lens among the first lensto the fifth lens has an object-side surface, which faces the objectside, and an image-side surface, which faces the image side; the opticalimage capturing system further comprises an aperture disposed before theimage-side surface of the second lens; wherein the optical imagecapturing system satisfies: 1.0≤f/HEP≤10.0; 0 deg<HAF≤50 deg; and|FS|≤15 μm; wherein f is a focal length of the optical image capturingsystem; HEP is an entrance pupil diameter of the optical image capturingsystem; HAF is a half of a maximum view angle of the optical imagecapturing system; for any surface of any lens; FS is a distance on theoptical axis between the first image plane and the second image plane.2. The optical image capturing system of claim 1, wherein a wavelengthof the infrared light ranges from 700 nm to 1300 nm, and the firstspatial frequency is denoted by SP1, which satisfies the followingcondition: SP1≤440 cycles/mm.
 3. The optical image capturing system ofclaim 1, wherein the optical image capturing system further satisfies:0.9≤2(ARE/HEP)≤2.0; wherein ARE is a profile curve length measured froma start point where the optical axis of the belonging optical imagecapturing system passes through the surface of the lens, along a surfaceprofile of the lens, and finally to a coordinate point of aperpendicular distance that is a half of the entrance pupil diameteraway from the optical axis.
 4. The optical image capturing system ofclaim 1, wherein the optical image capturing system further satisfies:IN23>IN34; wherein IN23 is a distance on the optical axis between thesecond lens and the third lens, and IN34 is a distance on the opticalaxis between the third lens and the fourth lens.
 5. The optical imagecapturing system of claim 1, wherein the optical image capturing systemfurther satisfies: IN23>IN45; wherein IN23 is a distance on the opticalaxis between the second lens and the third lens, and IN45 is a distanceon the optical axis between the fourth lens and the fifth lens.
 6. Theoptical image capturing system of claim 1, wherein the optical imagecapturing system further satisfies: 0<HOS/HOI≤1.6; wherein HOS is adistance between the object-side surface of the first lens and the firstimage plane on the optical axis, and HOT is a maximum image height onthe first image plane perpendicular to the optical axis.
 7. The opticalimage capturing system of claim 1, wherein the optical image capturingsystem further satisfies: 0.05≤ARE51/TP5≤25; and 0.05≤ARE52/TP5≤25;wherein ARE51 is a profile curve length measured from a start pointwhere the optical axis passes the object-side surface of the fifth lens,along a surface profile of the object-side surface of the fifth lens,and finally to a coordinate point of a perpendicular distance that is ahalf of the entrance pupil diameter away from the optical axis; ARE52 isa profile curve length measured from a start point where the opticalaxis passes the image-side surface of the fifth lens, along a surfaceprofile of the image-side surface of the fifth lens, and finally to acoordinate point of a perpendicular distance that is a half of theentrance pupil diameter away from the optical axis; TP5 is a thicknessof the fifth lens on the optical axis.
 8. The optical image capturingsystem of claim 1, wherein the optical image capturing system furthersatisfies: PLTA≤200 μm; PSTA≤200 μm; NLTA≤200 μm; NSTA≤200 μm; SLTA≤200μm; SSTA≤200 μm; and |TDT|≤50%; wherein TDT is a TV distortion; HOI is amaximum height for image formation perpendicular to the optical axis onthe image plane; PLTA is a transverse aberration at 0.7 HOI on the imageplane in the positive direction of a tangential fan of the optical imagecapturing system after a longest operation wavelength of visible lightpassing through an edge of the aperture; PSTA is a transverse aberrationat 0.7 HOI on the image plane in the positive direction of thetangential fan after a shortest operation wavelength of visible lightpassing through the edge of the aperture; NLTA is a transverseaberration at 0.7 HOI on the image plane in the negative direction ofthe tangential fan after the longest operation wavelength of visiblelight passing through the edge of the aperture; NSTA is a transverseaberration at 0.7 HOI on the image plane in the negative direction ofthe tangential fan after the shortest operation wavelength of visiblelight passing through the edge of the aperture; SLTA is a transverseaberration at 0.7 HOI on the image plane of a sagittal fan of theoptical image capturing system after the longest operation wavelength ofvisible light passing through the edge of the aperture; SSTA is atransverse aberration at 0.7 HOI on the image plane of a sagittal fanafter the shortest operation wavelength of visible light passing throughthe edge of the aperture.
 9. The optical image capturing system of claim1, wherein the optical image capturing system further satisfies:0.2≤InS/HOS≤1.1; wherein InS is a distance between the aperture and thefirst image plane on the optical axis, and HOS is a distance between theobject-side surface of the first lens and the first image plane on theoptical axis.
 10. An optical image capturing system, in order along anoptical axis from an object side to an image side, comprising: a firstlens having refractive power; a second lens having refractive power; athird lens having refractive power; a fourth lens having refractivepower; a fifth lens having positive refractive power; a first imageplane, which is an image plane specifically for visible light andlocated at a position of the optical axis with a through-focusmodulation transfer rate (value of MTF) at a first spatial frequencyhaving a maximum value at central field of view of the first imageplane, and the first spatial frequency being 110 cycles/mm; and a secondimage plane, which is an image plane specifically for infrared light andlocated at a position of the optical axis with a through-focusmodulation transfer rate (value of MTF) at the first spatial frequencyhaving a maximum value at central of field of view of the second imageplane, and the first spatial frequency being 110 cycles/mm; wherein theoptical image capturing system has a total of the five lenses withrefractive power; at least one lens among the first lens to the fifthlens has positive refractive power; each lens among the first lens tothe fifth lens has an object-side surface, which faces the object side,and an image-side surface, which faces the image side; the optical imagecapturing system further comprises an aperture disposed before theimage-side surface of the second lens; wherein the optical imagecapturing system satisfies: 1.0≤f/HEP≤10.0; 0 deg<HAF≤50 deg; |FS|≤10μm; and 0.9≤2(ARE/HEP)≤2.0; wherein f is a focal length of the opticalimage capturing system; HEP is an entrance pupil diameter of the opticalimage capturing system; HAF is a half of a maximum view angle of theoptical image capturing system; for any surface of any lens; FS is adistance on the optical axis between the first image plane and thesecond image plane; ARE is a profile curve length measured from a startpoint where the optical axis passes therethrough, along a surfaceprofile thereof, and finally to a coordinate point of a perpendiculardistance that is a half of the entrance pupil diameter away from theoptical axis.
 11. The optical image capturing system of claim 10,wherein the optical image capturing system further satisfies:IN23>11\34; wherein IN23 is a distance on the optical axis between thesecond lens and the third lens, and IN34 is a distance on the opticalaxis between the third lens and the fourth lens.
 12. The optical imagecapturing system of claim 10, wherein the optical image capturing systemfurther satisfies: IN23>IN45; wherein IN23 is a distance on the opticalaxis between the second lens and the third lens, and IN45 is a distanceon the optical axis between the fourth lens and the fifth lens.
 13. Theoptical image capturing system of claim 10, wherein the optical imagecapturing system further satisfies: 0<HOS/HOI≤1.6; wherein HOS is adistance between the object-side surface of the first lens and the firstimage plane on the optical axis, and HOI is a maximum image height onthe first image plane perpendicular to the optical axis.
 14. The opticalimage capturing system of claim 10, wherein the optical image capturingsystem further satisfies: 0.9≤ARS/EHD≤2.0; wherein, for any surface ofany lens, EHD is a maximum effective half diameter thereof, ARS is aprofile curve length measured from a start point where the optical axispasses therethrough, along a surface profile thereof, and finally to anend point of the maximum effective half diameter thereof.
 15. Theoptical image capturing system of claim 10, wherein the first imageplane and the second image plane are either flat or curved.
 16. Theoptical image capturing system of claim 10, wherein the optical imagecapturing system further satisfies: 0<IN45/f≤5.0; wherein IN45 is adistance on the optical axis between the fourth lens and the fifth lens.17. The optical image capturing system of claim 10, wherein the opticalimage capturing system further satisfies: 0.1≤(TP5+IN45)/TP4≤50; whereinIN45 is a distance on the optical axis between the fourth lens and thefifth lens; TP4 is a thickness of the fourth lens on the optical axis;TP5 is a thickness of the fifth lens on the optical axis.
 18. Theoptical image capturing system of claim 10, wherein at least one surfaceof each of at least two lenses among the first lens to the fifth lenshas at least an inflection point thereon.
 19. An optical image capturingsystem, in order along an optical axis from an object side to an imageside, comprising: a first lens having refractive power; a second lenshaving refractive power; a third lens having refractive power; a fourthlens having refractive power; a fifth lens having positive refractivepower; a first average image plane, which is an image plane specificallyfor visible light and perpendicular to the optical axis; the firstaverage image plane exists at an average position of defocusingpositions of the optical image capturing system, where through-focusmodulation transfer rates (values of MTF) of the visible light atcentral field of view, 0.3 field of view, and 0.7 field of view are attheir respective maximum at a first spatial frequency; the first spatialfrequency being 110 cycles/mm; and a second average image plane, whichis an image plane specifically for infrared light and perpendicular tothe optical axis; the second average image plane exists at the averageposition of the defocusing positions of the optical image capturingsystem, where through-focus modulation transfer rates of the infraredlight (values of MTF) at central field of view, 0.3 field of view, and0.7 field of view are at their respective maximum at the first spatialfrequency; the first spatial frequency being 110 cycles/mm; wherein theoptical image capturing system has a total of the five lenses havingrefractive power; at least one lens among the first lens to the fifthlens has positive refractive power; each lens among the first lens tothe fifth lens has an object-side surface, which faces the object side,and an image-side surface, which faces the image side; the optical imagecapturing system further comprises an aperture disposed before theimage-side surface of the second lens; wherein the optical imagecapturing system satisfies: 1≤f/HEP≤10; 0 deg<HAF≤50 deg; |AFS|≤20 μm;and 0.9≤2(ARE/HEP)≤2.0; wherein f is a focal length of the optical imagecapturing system; HEP is an entrance pupil diameter of the optical imagecapturing system; HAF is a half of a maximum view angle of the opticalimage capturing system; AFS is a distance on the optical axis betweenthe first average image plane and the second average image plane; ARE isa profile curve length measured from a start point where the opticalaxis passes therethrough, along a surface profile thereof, and finallyto a coordinate point of a perpendicular distance that is a half of theentrance pupil diameter away from the optical axis.
 20. The opticalimage capturing system of claim 19, wherein the optical image capturingsystem further satisfies: 0.5≤InS/HOS≤1.1; wherein InS is a distance onthe optical axis between the aperture and the first average image plane,and HOS is a distance between an object-side surface of the first lensand the first average image plane on the optical axis.
 21. The opticalimage capturing system of claim 19, wherein the optical image capturingsystem further satisfies: IN23>IN34; wherein IN23 is a distance on theoptical axis between the second lens and the third lens, and IN34 is adistance on the optical axis between the third lens and the fourth lens.22. The optical image capturing system of claim 19, wherein the opticalimage capturing system further satisfies: IN23>IN45; wherein IN23 is adistance on the optical axis between the second lens and the third lens,and IN45 is a distance on the optical axis between the fourth lens andthe fifth lens.
 23. The optical image capturing system of claim 19,wherein the object-side surface of the fourth lens on the optical axisis a concave surface, and the image-side surface of the fourth lens onthe optical axis is a convex surface.
 24. The optical image capturingsystem of claim 19, further comprising an image sensor, wherein theimage sensing device is disposed on the first average image plane andcomprises at least 100 thousand pixels; the optical image capturingsystem further satisfies: 0.5≤InS/HOS≤1.1; wherein InS is a distancebetween the aperture and the first average image plane on the opticalaxis; and HOS is a distance between an object-side surface of the firstlens and the first average image plane on the optical axis.